synthesis and characterisation of covalent organic ... · organic frameworks that were...
TRANSCRIPT
SYNTHESIS AND
CHARACTERISATION OF
COVALENT ORGANIC
FRAMEWORKS AS THIN FILMS
Nikka Maria Joezar Turangan
B. App. Sci.
Submitted in fulfilment of the requirements for the degree of
Master of Applied Science
School of Chemistry, Physics and Mechanical Engineering
Science and Engineering Faculty
Queensland University of Technology
2019
SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN FILMS i
Keywords
Covalent organic frameworks, COF, porous material, membrane, thin films, self-
supporting, freestanding, condensation reaction, reversibility, dynamic covalent
chemistry
ii SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN FILMS
Abstract
Covalent organic frameworks (COFs) were polymer assemblies formed from
light elements with high crystallinity, high porosity and configurable skeletal structure.
They have potential applications in filtration, gas storage, and electronic devices
among others. However, the realization of these applications requires a high degree of
morphological control in their preparation. The construction of substrate-confined
COF materials that were simultaneously highly crystalline, well-oriented and
functional remains a challenge due to the relatively small amount of work that has been
done to study the nucleation and growth of covalent organic frameworks, particularly
on a substrate. An understanding of COF growth in films is crucial to further progress
the development of more concrete techniques that will ultimately lead to covalent
organic frameworks that were crystallographically and structurally well-defined in
film form. A similar challenge exists around freestanding COF membranes,
which could be used for flow-through application or integrated to other systems. In
this thesis, a range of synthesis techniques to fabricate substrate-confined films were
explored, and procedures to create freestanding films were constructed. We began the
project with preliminary studies of known thin film synthesis methods that we then
adapted for precursor film fabrication. Through this we improved on the quality of
crucial parameters and further categorized our refined options based on different
strategies: thermal annealing and room temperature solvent-vapour annealing. These
intensive experiments led to the development of a procedure that requires no thermal
input for the creation of freestanding films. We found solvent choice and precursor
concentration to be the key parameters for film formation, whether substrate-confined
or self-supporting.
SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN FILMS iii
Table of Contents
Keywords .................................................................................................................................. i
Abstract .................................................................................................................................... ii
Table of Contents .................................................................................................................... iii
List of Figures ........................................................................................................................... v
List of Tables ............................................................................................................................ x
List of Abbreviations .............................................................................................................. xi
Statement of Original Authorship .......................................................................................... xii
Dedication ............................................................................................................................. xiii
Acknowledgements ................................................................................................................. xv
Chapter 1: Introduction ...................................................................................... 1
1.1 Background ..................................................................................................................... 1
1.2 Context............................................................................................................................ 2
1.3 Purpose ........................................................................................................................... 2
1.4 Significance, Scope and Definitions ............................................................................... 2
1.5 Thesis Outline ................................................................................................................. 3
Chapter 2: Literature Review ............................................................................. 5
2.1 What Makes a Porous Material? ..................................................................................... 5
2.2 Covalent Organic Frameworks ....................................................................................... 7
2.3 Covalent Organic Frameworks as Films ....................................................................... 12
2.4 Summary and Implications ........................................................................................... 16
Chapter 3: Research Design .............................................................................. 17
3.1 Experimental Design .................................................................................................... 17
3.2 Materials ....................................................................................................................... 18
3.3 Synthesis Approaches and Tools .................................................................................. 23
3.4 Characterisation of COFs ............................................................................................. 26
3.5 Parameters Explored Throughout Work…...………………………………………….28
Chapter 4: Results .............................................................................................. 29
4.1 Solvothermal Films ....................................................................................................... 29
4.2 Sonication ..................................................................................................................... 36
4.3 Spin-Coating ................................................................................................................. 39
4.4 Thermal Imprinting ....................................................................................................... 42
4.5 A Note on Analytical Techniques ................................................................................. 45
4.6 Conclusions .................................................................................................................. 46
iv SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN FILMS
Chapter 5: Substrate-Supported Membranes through Thermal Processing 49
5.1 Solvothermal ................................................................................................................ 49
5.2 Thermal Imprinting with Cyclohexanone Solution ...................................................... 55
5.3 Thermal Imprinting in the Presence of Water .............................................................. 58
5.4 Solvothermal Synthesis on Aluminium Foil ................................................................ 58
5.5 Conclusions .................................................................................................................. 61
Chapter 6: Substrate-Supported Membranes through Solvent-Vapour
Annealing 63
6.1 Solvent-Vapour Annealing at Room Temperature ....................................................... 63
6.2 Solvent-Vapour Annealing with Thermal Processing .................................................. 68
6.3 Conclusions .................................................................................................................. 71
Chapter 7: Self-Supporting COF-1 Membranes ............................................. 72
7.1 Synthesis Details .......................................................................................................... 72
7.2 Characterisation of the Freestanding Membranes ........................................................ 73
7.3 Discussion .................................................................................................................... 78
7.4 Conclusions .................................................................................................................. 80
Chapter 8: Conclusions ...................................................................................... 83
Bibliography ............................................................................................................. 88
Appendices .............................................................................................................. 100
Appendix A .......................................................................................................................... 100
Appendix B .......................................................................................................................... 102
Appendix C .......................................................................................................................... 104
Appendix D .......................................................................................................................... 105
Appendix E ……………………………………………………………………………….. 106
SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN FILMS v
List of Figures
Figure 1. Illustration of the conversion of the precursor molecule BDBA to
COF-1.1 Figure reproduced from Côté et al.1 with permission from
The American Association for the Advancement of Science. ....................... 8
Figure 2. Illustration of the conversion of the precursor molecules BDBA and
HHTP to COF-5. 1 Figure reproduced from Côté et al.1 with
permission from The American Association for the Advancement of
Science. .......................................................................................................... 8
Figure 3. Illustration of the preparation of a COF-1 membrane via the assembly
of exfoliated COF-1 nanosheets. 100 Figure reproduced from Li et al.100
with permission from the American Chemical Society. .............................. 13
Figure 4. ACOF-1 membrane on a porous α-Al₂O₃ support. 102 (a) illustration
of synthesis process; (b) Cross-sectional SEM image of synthesised
membrane. Figure reproduced from Fan et al. 102 with permission from
the Royal Society of Chemistry. .................................................................. 13
Figure 5. Structure of PEBA and SEM image of cross-section of TpPa-1-
nc/PEBA composite membrane synthesised by Schiff base
aldehyde−amine condensation.110 Figure reproduced from Zou et al.110
with permission from the American Chemical Society. .............................. 14
Figure 6. (A) Solution casting of colloid yields a coherent, free-standing COF
film. (B) Optical image of transparent freestanding COF-5 film. (C)
SEM of freestanding film.7 Figure reproduced from Smith et al.7 with
permission from the American Chemical Society. ...................................... 15
Figure 7. Project workflow map. ............................................................................... 17
Figure 8. SEM Images of the precursors (a) 1,4 -benzenediboronic acid
(BDBA) and (b) 2,3,6,7,10,11 -hexahydroxytriphenylene (HHTP)
powders ........................................................................................................ 18
Figure 9. The HOPG substrate in (a) photograph143 and (b) illustration of its
crystal structure143 ........................................................................................ 21
Figure 10. Graphene on Cu foil; (a) photograph of foil substrate,145 (b) Copper
foil morphology on graphene on copper foil imaged using SEM ................ 21
Figure 11. Photographs of (a) glass slide,146 (b) SiO2 on Si wafer,147 and (c)
ceramic crucible148 ....................................................................................... 22
Figure 12. SEM images of (a) Teflon (PTFE) and (b) ceramic filter paper
substrates ...................................................................................................... 22
Figure 13. Photograph of the spin-coater used for deposition of films. ..................... 23
Figure 14. Illustration of setup of the solvothermal synthesis ................................... 24
Figure 15. Illustration of the setup of the room temperature solvent-vapour
synthesis ....................................................................................................... 25
vi SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN FILMS
Figure 16. Schematic illustration of the thermal imprinter (a), and photograph
of the imprinter (b). ...................................................................................... 26
Figure 17. Crystallite distribution of drop-cast solovothermal samples imaged
usng SEM; (a) HOPG, (b) SiO2/Si wafer, and (c) graphene on Cu foil;
IR spectra in (d) of the post-synthesis crystallites with as-recieved
BDBA powder for comparison. ................................................................... 30
Figure 18. IR spectrum of solvothermally annealed crystallites and precursor
powder…………………………………………………………………......31
Figure 19. COF-1 crystallites imaged using a polarizing light microscope. (a)
sample prepared using heptanoic acid solution; (b) sample prepared
using heptanoic acid-ethanol solution. ......................................................... 32
Figure 20. COF-1 crystallites imaged using SEM. (a) sample prepared using
heptanoic acid solution; (b) sample prepared using heptanoic acid-
ethanol solution. ........................................................................................... 32
Figure 21. Heptanoic acid/ethanol solvothermal BDBA crystals high-resolution
imaged using helium ion microscopy; (a) layered crystal morphology
of the heptanoic acid/ethanol treated BDBA crystal; (b) close-up of
the crystal layers. ......................................................................................... 35
Figure 22. Crystal morphologies of BDBA crystals solvothermally synthesised
in various solvents imaged using SEM; (a) ethanol, (b) 0.5:1
heptanoic acid/ethanol, (c) 1:1 ethanol/acetone, (d) acetone . ..................... 35
Figure 23. Comparing two instances of sonication of graphene on Cu foil in a
vial of solution, with the second experiment using the same vial and
solution as well; (a) film morphology of first experiment; (b) close-
up of sparse crystal distribution; (c) film morphology of second
experiment; (d) close-up of crystal distribution. ........................................ 37
Figure 24. Film on various substrates synthesised via ultrasonication imaged
using SEM; (a) graphene on Cu foil and (b) HOPG. ................................... 38
Figure 25. Other crystal and particle morphologies observed on a post-
sonicated graphene on Cu foil imaged through SEM; (a) blocks of
crystals dispersed randomly on film; (b) crystals appearing to be
broken chunks of a much longer piece; (c) small crystals dispersed
randomly on more uneven regions of the substrates. ................................. 38
Figure 26. BDBA solution spin-coated on two different substrates imaged
using (a) HIM on the Si wafer and (b) SEM on the HOPG. ........................ 40
Figure 27. Comparison of films spin coated and then annealed on two different
substrates. (a-b) film on Si wafer imaged using (a) optical microscopy
and (b) helium ion microscopy. (c-d) film on HOPG imaged using (c)
optical microscopy and (d) scanning electron microscopy. ......................... 41
Figure 28. IR Spectra of thermally annealed spin-coated COF-1 film vs BDBA
precursor powder .......................................................................................... 41
Figure 29. SEM images of morphological variations of thermally imprinted
COF-1 films on Si substrates synthesised on four different days using
the same solution; (a) layering of crystals in various distractions; (b)
crystal mass appearing to be more fused together than in (a) due to
SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN FILMS
vii
greater impact from compression; (c) dense masses of crystals; (d)
densest packing of crystals seen in all samples. ......................................... 43
Figure 30. Thermally imprinted COF-1 film imaged using a stereomicroscope;
(a) spin-coated substrate, and (b) clean substrate. ....................................... 44
Figure 31. IR spectra of thermally imprinted COF-1 film and BDBA precursor
powder. ......................................................................................................... 44
Figure 32. Other morphologies observed on thermally imprinted COF-1 films
imaged using SEM; (a) leaf-like crystal growth; (b) uneven
distribution of pellet-shaped crystals; (c) sparse masses of crystal
aggregations. ................................................................................................ 45
Figure 33. COF-1 film on a Si wafer synthesised via thermal annealing imaged
using the stereomicroscope for (a) and (b) and SEM for (c); (a) film
morphology post-synthesis; (b) sponge-like underside of film; (c)
close-up of the underside of film. ............................................................... 50
Figure 34. COF-1 film on an HOPG substrate synthesised via thermal
annealing imaged using a stereomicroscope; (a) curled-films post-
synthesis; (b) close-up of films with spherical droplets visible. ................ 50
Figure 35. COF-1 film thermally annealed with distilled cyclohexanone imaged
using a stereomicroscope; (a) film morphology post-synthesis; (b)
sponge-like morphology of the underside of denser, more opaque
films. ............................................................................................................ 51
Figure 36. IR spectrum of COF-1 film obtained by thermal annealing with
BDBA powder for comparison. ................................................................... 51
Figure 37. COF-1 film synthesised on a ceramic crucible via thermal annealing
imaged using SEM; (a) Film morphology post-synthesis; (b) close-up
of crystal growth and fractures. .................................................................. 52
Figure 38. IR spectra of the surface, underside and powder form of the COF-1
film synthesised via thermal annealing on a ceramic crucible with
BDBA powder shown for comparison. ........................................................ 52
Figure 39. Film synthesised on a Teflon filter paper via thermal annealing
imaged using SEM. (a) continuous, smooth region of the film post-
synthesis; (b) porous, sponge-like crystal morphology dominant on
film; (c) cracks appearing to be influenced by the filter web texture;
(d) close-up of the cracks. ........................................................................... 53
Figure 40. IR spectrum of the film formed on teflon filter paper with BDBA
powder data for comparison. ........................................................................ 54
Figure 41. SEM images of BDBA film synthesised via solvothermal annealing
on a ceramic filter paper. (a) film morphology post-synthesis; (b)
close-up of the porous, sponge-like crystal morphology dominant on
the film; (c) partial coverage of film (right) on the filter paper. ................ 55
Figure 42. COF-1 film synthesised via thermal imprinting on an SiO₂ wafer
imaged using stereomicroscope in (a) and the SEM in (b), (c), and (d).
(a) film morphology post-synthesis; (b) spherical masses that make
up the 'holey' appearance in (a); (c) close-up of connected spherical
masses; (d) interwoven crystal growth in the less 'holey' regions. ............ 56
viii SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN
FILMS
Figure 43. Repeat experiment of COF-1 film synthesised via thermal
imprinting on an Si wafer imaged using stereomicroscope in (a) and
(b) and the SEM in (c), and (d). (a) film morphology post-synthesis;
(b) optical close-up of the droplet-like features; (c) details of the
droplets; (d) a variation of the droplet feature seen on a different
location on the same sample. ...................................................................... 57
Figure 44. IR spectrum of thermal imprinted film using the
cyclohexanone/ethanol/ether solution vs BDBA precursor powder to
show absence of peak shifts or conversion. ................................................. 57
Figure 45. COF-1 film synthesised via thermal imprinting with the presence of
water imaged using SEM. (a) crystal distribution post-synthesis; (b)
close-up of the web-like structure of crystals due to degradation. ............ 58
Figure 46. COF-1 film synthesised via solvothermal annealing on aluminium
foil with refined solution imaged using HIM and SEM. (a) film
morphology of film delaminated from the aluminium foil (in the
background); (b) close-up of flat region seen in (a); (c) layering of
crystals on the delaminated film; (d) fracture behavior of films still
adhered to aluminium foil. .......................................................................... 60
Figure 47. IR spectrum of COF-1 synthesised via solvothermal annealing on
aluminium foil with BDBA powder for reference. ...................................... 60
Figure 48. COF-5 film synthesised via room temperature solvent-vapour
annealing on a glass slide imaged using stereomicroscope in (a) and a
close-up in (b) and the SEM in (c), and a close-up in (d). ........................... 64
Figure 49. COF-5 film synthesised via room temperature solvent-vapour
annealing on a Si wafer imaged using stereomicroscope in (a) and a
close-up in (b) and the SEM in (c), and a close-up in (d) ........................... 65
Figure 50. IR spectrum of COF-5 film synthesised via solvent-vapour annealing and
the COF-5 solution.………………………………………………………..65
Figure 51. Crystal morphology of unsuccessful synthesis of COF-5 film via
room temperature solvent-vapour annealing imaged using imaged
using stereomicroscope in (a) and (b) and the SEM in (c), and (d). (a)
film morphology post-synthesis; (b) close-up of BDBA and HHTP
crystal combination; (c) close-up of crystal growth on edge of film;
(d) general crystal morphology. ….. ........................................................... 66
Figure 52. Film synthesised via room temperature solvent-vapour annealing on
an SiO₂ wafer imaged using stereomicroscope in (a), (b), and (c) and
the SEM in (d). (a) film morphology after synthesis; (b) close-up of
shield like film near the edge of substrate; (c) crystal morphology if
'shield' was absent; (d) close-up of the maze-like structure in (a). ............ 67
Figure 53. IR spectrum of film synthesised via solvent-vapour annealing at
room temperature with BDBA precursor powder for comparison............... 68
Figure 54. IR spectrum of the COF-1 film synthesised via thermal solvent-
vapour annealing with a BDBA powder precursor spectrum for
comparison. .................................................................................................. 69
SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN FILMS
ix
Figure 55. Surface distribution of COF-1 film synthesised on Si wafer via
thermal solvent-vapour annealing imaged using an (a) optical
microscope, and (b) polarizing microscope; Crystal (c) distribution
and (d) morphology imaged at high-resolution using SEM. ........................ 70
Figure 56. XRD spectra of COF-1 film synthesised on a Si wafer via thermal
solvent-vapour annealing. ............................................................................ 70
Figure 57. COF-1 self-supporting membranes synthesised via thermal
annealing and vapour annealing. (a) cross-section of bottom layer of
both membranes; (b) surface bottom layer of solvothermally annealed
membrane; (c) cross-section of top and bottom layer of vapour
annealed membrane; (d) surface of bottom layer of the vapour
annealed membrane; (e) surface of the top bottom layer of vapour
annealed; (f) stereo-optical image of surface of top layer of
solvothermally annealed membrane. ........................................................... 74
Figure 58. AFM phase images and roughness profile of (a) solvothermally
annealed COF-1 and (b) vapour annealed COF-1 membranes .................... 75
Figure 59. XRD spectra of solvothermally annealed (blue) membrane with a
sharper peak and less evidence of unreacted BDBA than the vapour
annealed (green) membrane. ........................................................................ 76
Figure 60. Clean Ar gas adsorption/desorption isotherms of TA (blue) and
vapour annealed (green) membranes. .......................................................... 77
Figure 61. Pre-degas (darker shade) and post-degas (lighter) FT-IR spectra of
TA (blue) and vapour annealed (green) membranes. ................................... 77
Figure 62. Nanoindentation loading curves for (a) TA COF-1 and (b) vapour
annealed COF-1 membranes with measurement spacing matrix in
onset. ............................................................................................................ 78
Figure 63. Setup of ultrasonic vibration assisted drop-casting. .............................. 100
Figure 64. Comparison of a COF film synthesised via room temperature
solvent-vapour annealing with solution drop-casted (a) and (b) with
assistance from ultrasonic vibrations and (c) and (d) without. .................. 101
Figure 65. Setup of COF-1 bulk powder synthesis via solvothermal processes. ..... 102
Figure 66. IR spectra of bulk powders synthesised via Côté’s1 procedure. ............. 103
Figure 67. Film and crystal morphology of COF-1 film synthesised via partial
solvothermal annealing and then plasma treatment. (a) film
morphology after plasma-treatment; (b) colour variations of crystals;
(c) white specks appearing to outline crystal shapes; (d) dendritic-
like darkening of crystals. ......................................................................... 104
Figure 68. Other crystal morphologies observed on a COF-1 film synthesised
via solvent-vapour annealing on a Si wafer. (a) crystal morphology
of overall film; (b) crystal morphology of the more homogenous
regions; (c) close-up of pointed edges of (b); (d) radiating
agglomerates of spindle-like crystals; (e) layered, intergrowth of
shell-like structures; (f) circular-disk shaped agglomerates of
crystals. ...................................................................................................... 105
x SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN FILMS
List of Tables
Table 1: Key Achievements in the Study of COFs .................................................... 10
Table 2: BDBA Solubility Table ................................................................................ 19
Table 3: Micropore-Mesopore Ratio of Surface Areas……………………………...79
Table 4: Syntheses in Chronological Order ............................................................... 84
SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN FILMS
xi
List of Abbreviations
COF Covalent organic frameworks
BDBA 1,4 -benzenediboronic acid / phenylenediboronic acid
HHTP 2,4,6,7,10,11 -hexahydroxytriphenylene
MOF Metal organic frameworks
COF-1 Covalent organic frameworks-1 (First COF created1)
COF-5 Covalent organic frameworks-5
PEBA Polyether block amide
VFET Vertical field-effect transistor
TTF Tetrathiafulvalene
PDBA Phenylenediboronic acid
NiPc Nickel phthalocyanine
BTDA Benzothiadiazole
PEDOT Poly(3,4-ethylenedioxythiophene)
DTPA Diethylenetriaminepentaacetic acid
FT-IR Fourier transform infrared spectroscopy
SEM Scanning electron microscope
HIM Helium ion microscope
XRD X-ray diffraction
HOPG Highly ordered pyrolytic graphite
SVA Solvent vapour annealing
AFM Atomic force microscopy
IR Infrared spectroscopy
TEM Transmission electron microscopy
BET Brunauer-Emmett-Teller
DFT Density functional theory
xii SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN
FILMS
Statement of Original Authorship
The work contained in this thesis has not been previously submitted to meet
requirements for an award at this or any other higher education institution. To the best
of my knowledge and belief, the thesis contains no material previously published or
written by another person except where due reference is made.
Signature:
Date: May 2019
QUT Verified Signature
SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN FILMS
xiii
Dedication
To Nicole.
xiv SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN
FILMS
SYNTHESIS AND CHARACTERISATION OF COVALENT ORGANIC FRAMEWORKS AS THIN FILMS
xv
Acknowledgements
I would like to thank my principal supervisor for her passion, enthusiasm and
endless guidance from the moment we first met back in my undergraduate years. Dr
Jennifer MacLeoad is without a doubt the reason writing the thesis, was a joy every
step of the way.
Thank you to my associate supervisor, Professor Steven Bottle for his generous
advices and constant reminder that chemists and physicists don't function the same
way, at all.
Thank you to my second associate supervisor, Dr Llewellyn Rintoul, for his
candor, philosophies on academia and memorable one-liners. And also for his
expertise like no other in IR, but that has always been part and parcel with Llew. His
no-nonsense attitude made me a better academic and I cannot be more grateful for
that.
Thank you to the CARF team for helping me monumentally with obtaining the
best data for my samples. They are what moves my project forward.
And last but not least, to the SEF and CPME HDR team. Thank you for
making my Masters journey a wonderful one and my PhD another endeavor I am
very much looking forward to begin.
Chapter 1: Introduction 1
Chapter 1: Introduction
1.1 BACKGROUND
Covalent organic frameworks (COF) are covalently-bonded organic materials
comprising the light elements boron, hydrogen, carbon and oxygen with high permanent
porosity due to their nanoporous structure. Many COFs are formed as 3D bulk crystals of
2D sheets, analogous to graphite/graphene. They were first synthesised by condensation
reactions of 1,4-benzenediboronic acid (BDBA) alone and with 2,3,6,7,10,11-
hexahydroxytriphenylene in 2005.1 In this synthesis, a closed reaction system was used to
maintain the presence of H2O, an essential factor to facilitating reversible bonding
conditions conducive to high-quality crystallite growth. The reaction progresses through
the formation of a boroxine ring and elimination of three water molecules and can be
reversed through the presence of excess water. Maintaining the presence of H2O is an
essential factor to facilitating the reversible conditions favourable to crystallite growth.2,3
The success of COF synthesis is based on overcoming the crystallization problem
in covalently bonded solids, wherein irreversible covalent bonds prevent error
correction.1,4 This can be avoided by balancing the relevant kinetics and thermodynamics
to promote reversibility of the bond formation, the key factor for extended crystalline
structures. Furthermore, the tunability of the chemical and physical properties of the
building-block molecules permits, in principle, controllable configuration of the material
structure.
Performing the condensation reaction in the presence of a graphene substrate leads
to staggered planar two dimensional sheets, roughly oriented with their basal planes
parallel to the surface, improving crystallinity compared to COF powders.5 In monolayer,
surface-supported form, COFs can be used in a range of applications. For example, they
can be used to template molecules through selective adsorption of molecules. This
characteristic can be utilised in sensing applications by maximizing the exposed active
area, and by increasing the thickness of the COFs from monolayer to multilayer.2
2 Chapter 1: Introduction
Here, we demonstrate a variety of approaches to creating COF films, both substrate-
bound and self-supporting. These methods provide a framework for easy tailoring of the
thickness, crystal size and pore size of the membranes. We characterize these films using
microscopy, x-ray diffraction, infrared spectroscopy, atomic force microscopy, and
nanoindentation. This type of understanding lays the groundwork for optimization of these
2D membranes, and their inclusion in applications, for example gas storage and filtration.
1.2 CONTEXT
Recent attention has turned to the synthesis of COFs beyond their original bulk
powder form and into nanosheets, composites, coating, gels, and membranes, targeting
applications such as molecular separations.6,2,7-10 This ability to synthesise freestanding
COF membranes brings us closer to applications where the COFs can be integrated into
engineered systems for, e.g., flow-through filtration applications. However, moving to
these applications requires the development of an understanding of the chemical, physical
and mechanical properties of these COF membranes, which are key to their successful use
in applications, particularly where the films may be required to self-support.
1.3 PURPOSE
The purpose of this study is to develop replicable and scalable (from nm to mm)
techniques for creating covalent organic framework thin films, both substrate-bound
and self-supporting.
1.4 SIGNIFICANCE, SCOPE AND DEFINITIONS
This project reports on the fabrication of COF beyond its original bulk powder
form, the challenges inherent in forming COF films, and implications for future
research in this field.
1.4.1 Thin Films and Membranes
The terms films, thin films, and membranes will be used interchangeably
throughout the thesis.
1.4.2 Silicon Wafer
Although the silicon wafer comprises a thin SiO2 native oxide layer on its
surface, the wafer will be defined simply as an Si wafer.
Chapter 1: Introduction 3
1.4.3 Room Temperature Solvent-Vapour Annealing
The terms solvent-vapour annealing, and vapour annealing will be used
interchangeably and is to mean vapour-assisted synthesis at room temperature. Vapour
annealing at other temperatures will be specified explicitly.
1.4.4 I/We
Use of “we” is a stylistic preference and refers to the single author of the thesis.
1.4.5 Scalable
The term scalable throughout the thesis unless otherwise stated is defined as
increasing the lateral length scale of the product film from the range of nm to
mm.
1.5 THESIS OUTLINE
Chapter 2 presents a literature review of covalent organic frameworks in their
many variations and forms, especially as thin films.
Chapter 3 details the experimental aspects of the project such as the materials,
experimental techniques and characterisation instruments used.
Chapter 4 describes the pilot studies undertaken to replicate bulk COF synthesis
techniques reported in the literature, and to characterize the resulting product. Can we
successfully synthesise a COF-1 film with the chosen methods? What parameters have
had the most influence?
Chapter 5 reports results on substrate-supported membranes synthesised through
thermal processing. Can we synthesise a mm scale COF-1 film through solvothermal
annealing? How does the solvent system chosen affect film growth and morphology?
Chapter 6 reports results on substrate-supported membranes synthesised through
solvent-vapour processing. Can we synthesise a mm scale COF-1 film through solvent
vapor annealing? How does substrate choice affect film growth and morphology?
Chapter 7 reports on the synthesis of self-supporting COF-1 membranes. What
were the resulting chemical, physical and mechanical properties of samples
synthesized via solvothermal annealing and solvent vapor annealing?
Chapter 8 closes the thesis and provides a brief deliberation on directions for
future work.
Chapter 2: Literature Review 5
Chapter 2: Literature Review
2.1 WHAT MAKES A POROUS MATERIAL?
The demands of society more often than not influence the development of
scientific knowledge and the functional materials imagined from this knowledge. The
concept of a porous material is one of them. Documented scientific research on
charcoal, a material dating back to the Ancient Egyptians,11 was not evident until the
18th century with the investigation of its adsorptive capabilities by Scheele, Priestley
and Fontana.12,13 At a similar time, Cronstedt14 discovered the frothing nature of a
stilbite he heated rapidly, naming the resulting mineral zeolite. Zeolite, a naturally
occurring and industrially produced mineral, is a common example of a porous
material/mineral that has been extensively studied due to its excellent physical and
chemical properties. Low production costs have made it an attractive material for a
wide range of applications, such as CO2 capture, water purification systems, and
oxygen concentrators.15-17 However, zeolites are susceptible to decreased performance
under humid conditions, are difficult to intrinsically fine-tune and functionalize, and
have low pressure capacity due to their small pore volume, posing a great obstacle to
widespread applications.18
Hence, interest in other types of engineered porous structures has grown in the
past decade due to their potential application in gas storage, nanotemplates and high
performance components of electronic devices.19,20 Organic thin films with porous
molecular structures have applications in technologies such as organic light emitting
diodes, to aid in maximising light emission through optical scattering21,22 and field-
effect transistors, for more efficient pathways for diffusion of gas molecules through
channels and hence improving overall performances such as on sensors.23,24 These
devices can potentially enable future low-cost electronics with uncompromised
performance, as they can be fabricated on cheap substrates such as glass and plastic,
and do not require capital-intensive manufacturing plants that are required for silicon-
based products. They can be fabricated using simple techniques such as screen-
printing, and spin-coating.25,26 Apart from cost, another important factor of increasing
interest is scalability. The advancement of technologies will depend on the shrinking
of micro-scale devices such as transistors (a 'top-down' approach), or building
6 Chapter 2: Literature Review
transistors molecule-by-molecule ('bottom- up'). Established microfabrication
techniques such as focused ion beam lithography or sputtering are top-down
approaches, and hence face physical limitations as they reach the molecular scale.27
Self-assembling molecules can overcome this problem as they can be incorporated into
bottom-up developments of nanostuctures. Self-assembly is based on molecules that
facilitate reversible non-covalent intermolecular bonds, resulting in long range ordered
structures.28 These bonds, however, are known to be weak and are easily
compromised, especially at increased temperature. The formation of covalent bonds
can overcome this problem, granting mechanically stable networked structures.29
The importance of ordering and control at the molecular level is also apparent in
other applications of organic films, such as electronics. The performance and
efficiency of electronic devices dramatically depend on the quality of the interface
between the electrodes and small-molecule molecular active layers that control the
carrier injection, a mechanism crucial to the fidelity of semiconductors in solid-state
electronics.30 Crystalline organic materials also have superior transport properties due
to their higher degree of molecular ordering.31 Increasing ordering in molecular films
is a key experimental challenge. Some of the ways include tuning of solvent system to
improve solvent-molecule interactions,32 or templating, where molecules adopt
positions consistent with the ordering on the template.33 A novel approach to this
problem has recently been reported: thermal imprinting is a form of nano imprint
lithography that involves the depositing a thin layer of solution in the substrate via
spin-coating and then brought into contact with a clean substrate and pressed together
with a calibrated pressure.34 This method was recently used to synthesise a
subphthalocyanine film with stable highly crystalline domains.35
Similar challenges exist for polymer films. Conductive polymers are widely used
in technologies such as solar cells, nano-fibers, liquid crystal displays and electrode
coatings due to their high stability, tunable electrical properties and low redox
potential. Conductive polymers, however, can have limited processibility,36,37
resulting in inhomogeneity in their films. The varying chain lengths, defects and chain
ends on these polymers contribute to the irregularity. Additionally, the chains can
orient in all three axes (x, y, z), giving each chain differing electronic properties. This
disorder leads to the localization of charges, affecting the overall electronic properties
of the film.38 Establishing deposition and synthesis conditions that allow for better
Chapter 2: Literature Review 7
control of the morphology and crystallinity is of great interest.
The search for materials that overcome the limitations inherent in zeolites, and
that may lead to the ordering necessary for incorporation of organic materials in a
range of applications led to the discoveries of metal-organic frameworks (MOFs) and
covalent organic frameworks (COFs), two prominent classes of porous crystalline
assemblies with high gas capture capacity and selectivity, good stability and
reusability, uniform pore sizes and low energy requirement for regeneration.18 COFs
are the material of interest in this thesis.
2.2 COVALENT ORGANIC FRAMEWORKS
Organic frameworks with covalent bonds can be obtained from reversible and
irreversible reactions. Irreversibility, however, leads to poor crystallinity or randomly
placed structures as there is no mechanism for correcting defects. This means that, in
most cases, long range order crystallinity cannot be achieved. Covalent organic
frameworks, on the other hand, are formed from reversible bonding processes,
allowing for error-checking and reduction or elimination of structural flaws until a
stable state is established.1,20 These organic materials are composed of building blocks
made from light elements such as boron, hydrogen, carbon, and oxygen and have high
permanent porosity due to their nanoporous structure. COFs can be formed as 3D
crystals comprising 2D sheets, analogous to graphite/graphene. The first COF, known
as COF-1, was synthesised by Yaghi and his team in 2005 through a condensation
reaction of the 1,4-benzenediboronic acid monomer, converging the boronic acid
molecules and eliminating water molecules to form a planar six-membered boroxine
ring (Figure 1). Yaghi and coworkers also demonstrated a second COF, COF-5, which
has two monomers, 1,4-benzendiboronic acid and hexahydroxytriphenylene, and is
formed through the dehydration reaction of the boronic acids and diols, resulting in a
five-membered borate ester ring as illustrated in Figure 2.8 A closed reaction system
was in place for both syntheses. This system maintains the presence of H2O, an
essential factor to facilitating reversible conditions conducive to high-quality
crystallite growth. In 2011, Colson et al.39 found that performing the condensation
reaction in the presence of a graphene substrate still led to the formation of the
boroxine ring but also resulted in staggered, planar two dimensional sheets roughly
oriented with their basal planes parallel to the surface, improving crystallinity
8 Chapter 2: Literature Review
compared to the COF powders produced by Côté et al.1
Because the backbone of a COF constitutes a periodic network, the design of
new COFs may start with determining the desired dimensionality of these systems,
either 2D or 3D, with research on both types of COF equally vast.40 Networks
extending in two dimensions are ultimately restricted to planar covalent bonds, and
generally have π-π stacking providing attractive intermolecular interaction between
the layered planes.41,42 A 3D network builds in all directions, resulting in a more
isotropic morphology, with the most common geometric net adopted for this structure
being the tetrahedron.43,44
Figure 2: Illustration of the conversion of the precursor molecules BDBA and HHTP to COF-5.
Figure reproduced from Côté et al. 1 with permission from The American Association for the
Advancement of Science.
Figure 1: Illustration of the conversion of the precursor molecule BDBA to COF-1. Figure
reproduced from Côté et al.1 with permission from The American Association for the
Advancement of Science.
Chapter 2: Literature Review 9
Considering that COFs comprise both linkages (bonding nodes) and struts
(organic spacers)20 the innovations in COF design can be broadly categorised.
Modification of the chemistry at the nodes allows control of the geometry, and has
been approached through reactions based on hydrazone,45-47 azine,48-51 triazine, based
on dynamic trimerization52,53 and more prominently, imine, which is generally based
on Schiff-based reactions.54-62 Modifications to the organic struts can add
functionality: the addition of a phthalocyanine63-67 introduces metal centers which can
enforce planarity and encourage an eclipsed stacking geometry that allows electron
delocalisation, facilitating charge carrier transport within the COF.64,65,67 Similarly,
porphyrins can be used to modify the band gap and enhance photocatalytic activity.68-
73 Tetrathiafulvalene (TTF), an organosulfur compound, has been integrated into a
porphyrin-based COF, boosting carrier transport and enhancing electric conduction.74
In monolayer, surface-supported form, COFs can also be used to template molecules,
and through selectively adsorption of molecules from solution. This characteristic can
be utilised in sensing applications by maximizing the exposed active area, and by
increasing the thickness of the COFs from monolayer to multilayer.12,13
The following is a summary, in chronological order, of the key achievements
that have been made since the birth of this class of materials. While there is an
abundance of evidence for rational synthesis through functionalization and geometry
control of organic molecules, strategies to fully control crystallite-scale morphology
and crystallographic orientation in films are still being established.
Table 1: Key Achievements in the Study of COFs
Year Achievement
2005 Synthesis of the first COFs, COF-1 and COF-5, via condensation reactions of
BDBA and HHTP.1
2006 Co-condensation of a linear alcohol with a triboronic acid (COF-18).75
2007 Extension of 2D hexagonal COFs by linking trigonal molecules, giving COF with
pore sizes between 9 and 32 (COF-6, COF-8, and COF-10).76
2007 Condensation of the zinc porphyrin tetraboronic acid with tetrahydroxybenzene,
producing COF-108, one of the most porous COFs with the lowest density.77
10 Chapter 2: Literature Review
2008 Condensation of borosilicate clusters (Pyrex) producing thermally and chemically
stable 3D COFs.78
2009 Utilisation of electroactive organosilane precursors with a surfactant-templated
synthesis to create porous hole-conducting framework material.79
2009 Synthesis of highly ordered conjugated pyrene COF using the co-condensation
reaction of triphenylene HHTP and pyrenediboronic acid (PDBA), giving a
hexagonal framework with eclipsed arrangements.80
2010 Reaction of tetragonal phthalocyaninetetra(acetonide) with a linear diboronic acid
and Lewis acid to form a tetragonal lattice.67
2011 A metallophthalocyanine COF and a porphyrin-based COF was synthesised,
creating a photoconductive COF which exhibits high charge carrier mobilities and
broad absorption profile.65
2011 Dehydration reactions produced hydrazone linked COFs.45
2011 COF with accessible pores of 4 nm was achieved.81
2011 Condensation reaction of porphyrin via a boronate ester formation (COF-66) or
imine bond formation (COF-366), producing macrocyclic COFs exhibiting
superior semiconductor properties.73
2011 Electron-transporting COF synthesised through substitution of benzene groups in
NiPc-COF electron deficient benzothiadiazole (BTDA) units.64
2012 Functionalization of 3D COFs using a monomer-truncation strategy.82
2013 Squaraine-based COF was produced.72
2014 Covalent TTF lattice through integration of TTF units to form 2D COFs.74
2014 Vapour-assisted synthesis of COF without a substrate, resulting in a nanofibrous
morphology.83
2015 An azine-linked COF was synthesised under solvothermal condition.50
Chapter 2: Literature Review 11
2015 Room-temperature vapour-assisted synthesis of COF-5, resulting in films < 10
microns thick.84
2016 Through imine-condensation reactions, a 3D COF with the ability to mutually
weave periodically was produced from helical organic threads.85
2016 Proposed condensation systems that utilises one knot and multiple linker units to
synthesise 2D and 3D multiple-component COFs.86
2016 Proposed the utilisation of aggregation-induced emission mechanism to create
highly emissive COFs.87
2016 The growth of the poly(3,4-ethylenedioxythiophene (PEDOT) conductive polymer
inside the pores of the COF to enhance transport and electrical capacities.88
2017 Stable colloidal suspensions of 2D COF particles were produced under
homogeneous 5polymerization conditions that prevented crystallite precipitation.6
2017 Growth of full-conjugated 2D COF on a dielectric hexagonal substrate.30
2017 Synthesis of ultraporous COF of various shapes through an ancient terracotta
process was demonstrated.57
2018 Layer-by-layer synthesis of imine-linked COF on a porous ultrafiltration membrane
with tunable thickness and unprecedented water permeance.89
2018 Interfacial polymerization of flexible COF thin films that possess exceptional
mechanical strength and durability in high humidity environment.90
2018 Phase transformation from compressive loading of COF grown on a porous DTPA
sheet observed through simulation models.91
2018 Study on the effect of water adsorption on CO₂ capture on COFs using monte carlo
simulations.92
2018 Etched-off copper assisted thermal conversion of COF capsules for metal-free
electrode materials.93
2018 Oil-confined interfacial synthesis of transferable COF films.94
12 Chapter 2: Literature Review
2.3 COVALENT ORGANIC FRAMEWORKS AS FILMS
Organic compounds have a prominent place in modern material science, whether
in fundamental research or commercialization.95 Natural abundance of precursors
(e.g., carbon) and low production cost are just some of the advantages over their
inorganic counterparts. Hence it may be no surprise that the majority of membranes
manufactured for research and commercial use are organic polymers.96-98 In addition
to the aforementioned advantages, they are easy to prepare and can be tailored for
specific functions. These membranes, however, cannot compete with their inorganic
or metallic counterparts when it comes to resistance to high temperature and harsh
chemicals. COFs synthesised in film form may be able to overcome these obstacles.
COF films can be directly grown on -Al2O3 ceramic substrates. The first two
COFs synthesised, COF-1 and COF-5, were successfully grown as nanosheets and
micron scale membranes respectively on these ceramic supports.99,100 The exfoliation
method used is presented in Figure 3. Other variants of COFs, both 2D9,101,102 and
3D103 have also been synthesised on -Al2O3 substrates and tested for gas separation
and capture with excellent long-term stability. An illustration of the synthesis of
ACOF-1 is given in Figure 4(a) and the synthesised product in Figure 4(b).101 When
applied as a coating layer on a ceramic separator, Wang et al.104 found that a COF
produced dramatically improved cycling performance of a lithium-sulfur battery.
Figure 3. Illustration of the preparation of a COF-1 membrane via the assembly of exfoliated COF-1
nanosheets. Figure reproduced from Li et al. 100 with permission from the American Chemical Society.
Chapter 2: Literature Review 13
Other substrates have also been demonstrated as suitable supports for COFs.
Medina et al.84 employed a room temperature solvent-vapour technique to grow COF-
5 on SiO2 substrates, resulting in micron-scale films. Another type of COF, a hybrid
of COF and metal-organic framework (MOF), was modified with polyaniline and
grown on SiO2 for potential H2/CO2 separation.105 COFs can also be synthesised on
fibrous substrates such as filter paper or soft cloth.106 Colson et al.39 grew COF-5 on
single-layer graphene substrates, producing oriented films ~75 nm thick. More
recently, an imine-linked COF was used as the transport channel layer on top of the
single-layer graphene source electrode in a vertical field-effect transistor (VFET),
giving exceptional ambipolar charge transport behaviour due to improved crystallinity
and controllable orientation.107
In addition to films supported on substrates, COFs have been integrated into
mixed matrix membranes, which are made of homogenously harmonized polymeric
and/or inorganic particle matrices.108 The incorporation of COFs as one of the
polymeric components results in a membrane with exceptional gas separation,108-116
liquid separation,116,117 desalination118 and intrinsic proton conduction119 capabilities.
A polyether block amide (PEBA)-based COF nanosheet synthesised via Schiff-based
condensation is shown in Figure 5. Other interesting membrane structured materials
that have been functionalised with COFs include tyrene-butadiene rubber,120
Figure 4. ACOF-1 membrane on a porous α-Al₂O₃ support. (a) illustration of synthesis process; (b)
Cross-sectional SEM image of synthesised membrane. Figure reproduced from Fan et al. 101 with
permission from the Royal Society of Chemistry.
(a)
(b)
14 Chapter 2: Literature Review
polybenzimidazole,121 membrane electrode assembly pellets,122 alumina tubes123 and
elastomers.124
While the benefits of integrating COFs into multicomponent membranes are
evidently numerous, there is also great interest in freestanding COF membranes.
Unlike the substrate-bounded alternative, self-supported membranes are transferrable
and can be integrated into various geometries.
A number of studies have demonstrated the solution-based synthesis or
exfoliative isolation of nanosheets.6,125-133 The colloid-based synthesis of freestanding
COF-5 nanosheets is illustrated in Figure 6. There are however, limitations to
exfoliation such as control of the thickness, limitations to sheet size and presence of
residual surfactants or solvents adsorbed into the sheets.134,135 However, work on
micron scale self-supporting COF membranes is has only emerged in recent
years. These membranes have the advantage of withstanding harsh chemicals and,
depending on the synthesis technique, can be scalable. Sasmal, et al.136 fabricated a
self-standing flexible COF membrane that facilitates superprotonic conductivity. A
palladium-loaded COF deposited into PTFE molds and then irradiated with UV light
produced freestanding membranes that proved to be functional for room temperature
chlorobenzene dechlorination in water137.
Figure 5. Structure of PEBA and SEM image of cross-section of TpPa-1-nc/PEBA composite membrane
synthesised by Schiff base aldehyde−amine condensation. Figure reproduced from Zou et al. 110 with
permission from the American Chemical Society.
Chapter 2: Literature Review 15
This ability to synthesise freestanding COF membranes with thicknesses on the
micron scale, brings us closer to applications where the COFs can be integrated into
engineered systems for, e.g., flow-through filtration applications. However, moving to
these applications also requires the development of an understanding of the mechanical
properties of these COF membranes, which are key to their successful use in
applications, particularly where the films may be required to self-support.
2.4 SUMMARY AND IMPLICATIONS
When combined with their robustness, porosity and potentially excellent
electronic properties, crystallographic control in COFs is a key ingredient to both
innovative and impactful nano-applications. However, there is still much to gain in our
understanding of the basic mechanisms controlling the assembly of covalent organic
frameworks. This knowledge is crucial to further progress the development of
techniques that will ultimately lead to covalent organic frameworks that are
crystallographically and structurally well-defined in film form, whether substrate-
confined or freestanding. When control and tunability of the properties of these films
is achieved, it will, in principle, pave the way to new functionalities and applications.
Figure 6. (A) Solution casting of colloid yields a coherent, freestanding COF film. (B) Optical image
of transparent freestanding COF-5 film. (C) SEM of freestanding film. Figure reproduced from
Smith et al.6 with permission from the American Chemical Society.
16 Chapter 2: Literature Review
Chapter 3: Research Design 17
Chapter 3: Research Design
3.1 EXPERIMENTAL DESIGN
Figure 7 details the typical experimental workflow of this project. We began with a
survey of published work for techniques that could be adapted to synthesizing COF-1 on
a substrate. Suitable strategies were selected and enacted. Once synthesised, each film
was then analysed using infrared spectroscopy to determine if conversion of the precursor
to COF-1 was successful. The experiment was deemed successful if conversion was
Determine crucial
parameters
Translate protocols
to produce self-
supported
membranes
Morphological
(SEM, HIM,
optical)
Chemical (FT-IR) Physical (XRD,
gas adsorption,
nanoindentation)
Adapt to convert
precursor to COF-1
substrate-confined
film
Identify/Refine
techniques from
published work
Figure 7. Project workflow map.
18 Chapter 3: Research Design
observed through shifts and attenuations of the boronic acid-related bands (B-O for
boronate ester, B₃O₃ for boroxine anhydride, and C-O for boroxoles); these bands will be
identified in IR spectra throughout the thesis. We could also roughly estimate COF-1
concentration through the ratio between the BDBA precursor bands and the evolved COF-
1 bands. XRD spectra can be similarly analysed, and ideally can provide quantitative
estimates not possible from IR spectra. The following chapters will discuss these spectral
data in further detail.
Whether an experiment was successful or not, analysis on film morphology was
performed for record keeping. We then returned to identifying a different technique or
refining the technique for further experiments.
Following a successful synthesis, and after morphology analysis, we examined the
film further for its physical properties through XRD, gas adsorption and nanoindentation
where possible. We then analysed the collected data and determined the crucial parameters
for successful translation of the protocol to the synthesis of self-supporting membranes.
3.2 MATERIALS
3.2.1 Chemicals
In this work, we chose to focus almost exclusively on the well-established COF
known as COF-1 as it was the pioneering COF, and is constituted by a single monomer,
1,4-benzenediboronic acid. We additionally made some studies on COF-5, which contains
two monomers, to follow exactly the synthesis strategies described in the literature for
(b)
(a)
Figure 8. SEM Images of the precursors (a) 1,4 -benzenediboronic acid (BDBA) and (b) 2,3,6,7,10,11 -
hexahydroxytriphenylene (HHTP) powders
10 µm
10 µm
Chapter 3: Research Design 19
solvent-vapour annealed films. The monomers, 1,4-benzenediboronic acid (BDBA, 95%)
and 2,3,6,7,10,11 -hexahydroxytriphenylene (HHTP, 95%) were purchased from Sigma
Aldrich and Tokyo Chemicals Industry, respectively, and were used as received. Figure 8
shows scanning electron microscopy (SEM) images of the precursor molecular powders.
COF synthesis involves dissolution of precursor molecules into solvent, and one of
our objectives in this work was to investigate and optimize solvents and solvent mixtures.
Ethanol (99.5%) and diethyl ether (99%) were purchased from Univar, cyclohexanone
(99%) from M&B Chemicals, cyclopentanone (99%) from ACROS Organics and
heptanoic acid (96%) from Sigma Aldrich. Except for the cyclohexanone, which was
distilled and then filtered, the solvents were used as received.
3.2.2 Solubility of precursors
A basic solubility test was completed by dissolving 10mg of BDBA in 1.5 mL of
solvent and is presented in Table 2. This investigation allowed us to formulate new solvent
systems that helps with the uniform deposition and synthesis of the precursor on the
chosen substrate.
Table 2: BDBA Solubility Table
Solvent
Solubility
of 10mg
BDBA
Appearance
Boiling
Point
(oC) 138-
140
Density
(g/mL)
138-140
Vapour
Pressure
20oC
(hPa) 138-
140
Viscosity
10¯³ Pa
s138-140
Formula1
38-140
1-methyl-2-
pyrrolidinone Complete
Powder
dissolved
easily
202 1.028 32 1.67 C₅H₉NO
2-butanone Mildly Cloudy 79.6 0.805 105 0.41 C4H8O
2-methoxyethanol Complete
Powder
dissolved
easily
124 0.965 6 1.72 C₃H₈O₂
Acetone Mildly Cloudy 56.2 0.786 240 0.3 C3H6O
Acetonitrile Mildly Cloudy 81.6 0.786 97 0.34 C2H3N
Acetyl acetone Mildly
Complete
after
sonication
140.4 0.975 3 - C5H8O2
Anisole Mildly Cloudy 153.7 0.996 3.5 - C7H8O
Chloroform Mildly
Powder
remains on
surface of
solvent
undissolved
61.2 1.498 210 0.54 CHCl3
Cyclohexanone Mildly Clumpy 155.6 0.948 5 2 C6H10O
Cyclopentanone Mildly
Complete
after
sonication
130.6 0.95 11.5 1.29 C5H8O
20 Chapter 3: Research Design
Dichloromethane Mildly
Some powder
remains on
surface of
solvent
undissolved
39.8 1.326 475 0.42 CH2Cl2
Diethyl ether Insoluble
Solvent stays
clear with no
powder
dissolved
34.6 0.713 587 0.22 C4H10O
Dimethyl sulfoxide Complete
Powder
dissolved
easily
189 1.092 0.61 2 C2H6OS
Dimethylacetamide Complete
Powder
dissolved
easily
165 0.937 300 0.945 C₄H₄NO
Dimethylformamide Complete
Powder
dissolved
easily
153 0.944 3.5 0.8 C₃H₇NO
Dioxane Complete
Powder
dissolved
easily
101.1 1.033 41 1.18 C4H8O2
Ethanol Complete
Powder
dissolved
easily
78.5 0.789 59 1.08 C2H6O
Ethyl acetate Mildly Cloudy 77 0.894 97 0.43 C4H8O2
Ethylene glycol Mildly Cloudy 197 1.115 0.092 16.1 C2H6O2
Heptanoic acid Mildly Cloudy 223 0.912 1.35 5 C7H14O2
Hexane fraction Mildly Clumpy 69 0.655 160 0.29 C6H14
Isopropanol Mildly
Complete
after
sonication
82.4 0.785 44 2.07 C₃H₈O
Methanol Complete
Powder
dissolved
easily
64.6 0.791 128 0.54 CH4O
Tetrahydrofuran Complete
Powder
dissolved
easily
66 0.886 200 0.46 C4H8O
Toluene Mildly Cloudy 110.6 0.867 29 0.55 C7H8
Trichlorobenzene Insoluble
Solvent stays
clear with no
powder
dissolved
213 1.46 1 0.562 C6H3Cl3
p-Xylene Mildly Cloudy 138.3 0.861 15 0.65 C8H10
Effects of concentration
To investigate the effect of monomer concentrations on distribution and
homogeneity on the substrate, we varied the solution concentrations in different trials,
ranging between 0.004 M to 0.22 M. This will be discussed throughout the thesis.
3.2.3 Substrates
The choice of substrate has a profound effect on growth and molecular ordering of
the film, allowing for different film functionalities and applications when selected
carefully.141
Chapter 3: Research Design 21
Crystalline substrates
Using crystalline substrates creates the platform for ordered epitaxial growth and
through control of the adsorption geometry of precursors. These effects contributed to the
success that Colson et al. achieved in growing ordered COF films.39,63 The highly oriented
pyrolytic graphite (HOPG) is a synthetic graphite that is highly ordered.142 The HOPG we
used was obtained from NT-MDT. The graphene on Cu foil is an alternative graphite-
based substrate that is less brittle and more flexible than the HOPG. The copper foil also
has a texture (Figure 10) that we have found to not have significant effect on the final
synthesis product.
20 µm
Figure 9. The HOPG substrate in (a) photograph143 and (b) illustration of its crystal structure.144
(a)
(b)
Figure 10. Graphene on Cu foil; (a) photograph of foil substrate, 145 (b) Copper foil morphology on
graphene on copper foil imaged using SEM
20 µm
(a)
(b)
22 Chapter 3: Research Design
Amorphous rigid substrates
Amorphous solids are non-crystalline materials without an ordered lattice pattern.
Despite this irregularity, they are flat, cheap and suitable for the synthesis of our films.
The glass slides were purchased from Sail Brand, the SiO2 on Si wafer from Ted Pella and
the ceramic crucible from ProSciTech (Figure 11).
Amorphous flexible substrates
Aluminium foil has the advantage of low cost, flexibility and scalability. It also
allows for easy removal of films. The aluminium foil used in this work is from Oso.
Filter materials
Filter paper provide for a substrate that is porous and unlike the others above. It is
interesting to see the effect of the porosity on the porous COF. The Teflon filter paper
(Figure 12(a)) was purchased from Advantec and the ceramic filter paper (Figure 12(b))
from Whatman.
Figure 12. SEM images of (a) Teflon (PTFE) and (b) ceramic filter paper substrates
10 µm
10 µm
10 µm
10 µm
(a)
(b)
Figure 11. Photographs of (a) glass slide, 146 (b) SiO2 on Si wafer, 147 and (c) ceramic crucible148
(a)
(b)
(c)
Chapter 3: Research Design 23
3.3 SYNTHESIS APPROACHES AND TOOLS
3.3.1 Deposition of precursor solution: drop casting
One of the most straightforward thin film synthesis techniques, drop-casting
involves the deposition of solution on a substrate usually using a pipette, dropper or
syringe. Surface tension between substrate and the solution plays one of the most
significant roles in the uniformity of the final synthesised products.
3.3.2 Deposition of precursor solution: spin coating
Spin coating is a commonly used technique for uniform thin film fabrication
where the film solution is deposited at the centre of a substrate that is fixed to a
spinning disk with configurable speed and acceleration settings. Upon contact with the
substrate, centrifugal force spreads the solution outward in all directions, coating the
surface uniformly. Continued rotation forces excess solution off the substrate, hence
thickness can be adjusted based on this parameter and also others such as viscosity and
volatility of the solvent(s) used in the solution and the speed setting itself.
A substrate was fixed using carbon tape (smaller than the substrate) on to a glass
slide cut to fit the suction hole on the spin-coater. The speed settings are detailed in
the appropriate chapter.
Figure 13. Photograph of the spin-coater used for deposition of films.
24 Chapter 3: Research Design
3.3.3 COF synthesis via solvothermal treatment
Solvothermal annealing involves the use of solvent or solvents to facilitate
synthesis of the precursor molecules through their interactions at relatively high
temperatures. Precise control of the final product can be achieved through
solvothermal synthesis due to the wide range of parameters that can be of influence:
temperature, temperature gradient, pressure, humidity, solvents, time, substrate,
substrate size, solution, solution deposition method, etc. The solvothermal setup for
our work is shown in Figure 14. The petri dish sufficiently seals the beaker and
becomes a closed, condensing environment with heating, eventually leading to heating
of the substrate and solution on the substrate. The temperature of 120 °C was initially
derived from Côté et al.’s synthetic procedure1 but was then adjusted to 115 °C as it
was found (through trial and error) to be the most ‘comfortable’ temperature for our
solvent system, ie, no burn stains or excessively rapid evacuation of solvents.
3.3.4 COF synthesis via solvent-vapour annealing
In solvent vapour annealing (SVA), the sample is exposed to a vapour of a
chosen solvent to induce polymerisation or ordering (curing) using the setup in Figure
15. This key aspect of this method is the gentle and consistent application of the
activating agent (vaporizing solvent) on to the sample. The main driver of
solvothermal annealing, on the other hand, is the high temperature input. This
energetic input is intense and abrupt, forcing chemical reactions to proceed at a fast
Sample substrate
Hotplate
Silica gel with
H₂O
2L beaker
Glass petri dish
Figure 14. Illustration of setup of the solvothermal synthesis
Chapter 3: Research Design 25
pace; in our experiments, thermal annealing took two hours compared to the 48-72
hours that is required to complete synthesis using solvent vapour annealing. Vapour
annealing is used either on its own or as a complementary technique in various fields
to produce block copolymers149 or materials suitable for photovoltaic
applications150,151. For the fabrication of COFs, vapour annealing has been utilised
twice, both at room temperature to create COF-5 as a thin film,93 and a nanofibrous
COF in bulk form.92 We attempted to emulate the former synthetic procedure and will
be discussed in Chapter 6.
3.3.5 COF synthesis via sonication
Sonochemical synthesis, or sonication, is the use of high intensity ultrasound to
form acoustic cavitation in liquids, where the energy produced is then used to initiate
chemical processes and reactions. The collapse of these cavitation bubbles leads to
local heating, intense pressures, drastic temperature gradients, and jet streams.152
These dramatic effects must be considered along with the increasing overall
temperature of the water bath, and hence the system, as the procedure progresses. This
technique has become particularly utilised in pharmaceutical research for its
effectiveness in particle emulsification, activation and deagglomeration.153 The
synthetic procedure involves the submersion of substrate in a sealed container (4 mL
vial) of the precursor solution for a given time. We found 2 hours to be the right
duration to observe growth on the substrate.
2L beaker
Parafilm
20mL beaker of anisole
Figure 15. Illustration of the setup of the room temperature solvent-vapour assisted synthesis
Silica gel
without H₂O
Sample substrate
26 Chapter 3: Research Design
3.3.6 Thermal imprinting
Thermal imprinting utilises mechanical deformation to aid in the thermal curing
of the solution drop-casted on the substrate. While this nanolithography derived
method usually involves the use of a template,154,155 this experiment only intend to take
advantage of the effects of pressure and compression on thin film growth. We start
with a spin-coated sample which is then immediately placed in the imprinter with a
clean substrate placed directly on top of it, face down as shown in Figure 16.
3.4 CHARACTERISATION OF COFS
3.4.1 Microscopy
High-resolution images of the COF membranes were obtained with both the
Zeiss Orion NanoFab Helium Ion Microscope (HIM) and Zeiss Sigma Scanning
Electron Microscope (SEM). For sample preparation, the membranes were adhered to
a carbon tape on an SEM specimen stub. An electron flood gun was utilised to
minimize sample charging. Optical images were captured using the Nikon SMZ1500
stereomicroscope and polarised images with the Leica DM6000. Tapping mode atomic
force microscopy (AFM) on a Park NX10 AFM was employed to image the surface
and profile the roughness of membranes obtained through both synthesis methods.
(b)
(a)
Figure 16. Schematic illustration of the thermal imprinter (a), and photograph
of the imprinter (b).
Chapter 3: Research Design 27
3.4.2 Spectroscopy
Fourier transform infrared (FT-IR, or IR) spectra were collected using the
Nicolet iS50 FTIR spectrometer with 64 scans at 4 cm-1 resolution. No difference in
quality was seen at 128 scans. Analysis on each sample was performed at least twice
to ensure consistency. Data were collected with respect to transmittance %. For
thermally processed samples, the sample was cooled down to room temperature in a
desiccator prior to analysis. Only films that were easily removed that had already
delaminated from the substrate were analysed without the substrate as forced removal
can cause the substrate to chip and contaminate the sample.
3.4.3 Surface area analyses
Surface area analyses were performed on the Micromeritics 3 Flex Physisorption
analyser using argon and at a pressure range between 0.01-0.1 p/p. The free space
values were determined at the end of the analysis instead of beginning to prevent
helium entrapment in the samples.
3.4.4 X-ray diffraction
2Θ and 1° fixed incident angles were used to acquire XRD measurements with
a Rigaku SmartLab diffractometer using a Cu Kα source. Data were fitted using the
Le Bail routine.
3.4.5 Nano-mechanical characterisation
Mechanical analysis of the membranes were performed with a Bruker Hysitron
TI 950 TriboIndenter with a cube corner tip and 1D transducer. A 2000 μN load
function was used, as determined through preliminary load testing of the sample.
Calculated modulus and hardness take into account substrate effects, probe shape and
tip and optical calibrations.
3.4.6 Transmission electron microscopy
Transmission electron microscopy (TEM) is a technique that utilises an electron
beam transmitted through the sample to form an image at high atomic resolutions.
28 Chapter 3: Research Design
3.5 PARAMETERS EXPLORED THROUGHOUT WORK
A synopsis of the variables explored is provided in Appendix E.
Chapter 4: Results 29
Chapter 4: Results
A series of pilot studies were performed to establish the fundamental parameters
necessary for transferring synthesis procedures originally designed for bulk and single-
layer COF-1s into thin film forms. The success of this relegation depends critically on
solvent wettability, solution evaporation rates, substrate choice, and the technique itself.
4.1 SOLVOTHERMAL FILMS
To determine the parameters most relevant in controlling COF film synthesis, we
started by considering the synthesis technique proposed by Côté et al. in 2005.1 In this
case, the self-condensation or molecular dehydration reaction of the 1,4-benzenediboronic
acid (BDBA) building block leads to the formation of bulk COF-1, a long-range-ordered
2D framework and the pioneering COF. The reaction involves the convergence of three
boronic acid molecules to form a boroxine ring and eliminate three water molecules. Côté
et al.’s solvent choice was a 1:1 mixture of mesitylene and dioxane.1 However, since we
were synthesising a film, we also considered the method conceived by Cui et al. in 2015.5
Heptanoic acid was used as the dissolving solvent for HOPG-confined synthesis of COF-
1.
For the pilot study, we started with a solution of 1 mg of the 1,4 benzenediboronic
acid (BDBA) monomer and 1.5 mL of heptanoic acid in a 4 mL vial. The solution was
then placed in an ultrasonic bath for 20 minutes to completely dissolve the BDBA
powders. In our first experiment, we drop-casted the solution onto a HOPG substrate and
proceeded with the classic solvothermal synthesis in a humid environment (see Section
3.3.3). The SEM image in Figure 17(a) shows the sample post-synthesis. Figure 17(b) and
(c) shows the result on other substrates: an Si wafer (b) and on a graphene on Cu foil
substrate (c). Consistent on all three substrates is the presence of crystallites relatively
evenly distributed across the surface. The HOPG and graphene on Cu foil also illustrate
the effect of an uneven or protruding surface on crystal seeding and nucleation. Crystal
30 Chapter 4: Results
seeding is based on the notion that recrystallisation starts when two random soluble
molecules suspended in a solute interact to create intermolecular forces that leads to the
formation of a basic crystal lattice. This lattice collides with another random molecule and
is extended, and so on. By placing a larger, formed crystal, or a seed, and in the case of
the HOPG and graphene on Cu foil substrates, the elevated textures, the reliance and time
required for random molecule interaction is eliminated. Based on Cui et al.’s results,5 we
assumeed that any evidence of COF monolayer formation is inappreciable at this
magnification and that the crystallites were either residual/unreacted BDBA or COF that
settled as isolated aggregates. It was determined through the infrared spectroscopy shown
in Figure 17(d) that these crystals were the former: BDBA crystallites precipitated out of
the heptanoic acid solution and were left unreacted on the surface of the substrate.
Figure 17. Crystallite distribution of drop-cast solovothermal samples imaged usng SEM; (a) HOPG,
(b) SiO2/Si wafer, and (c) graphene on Cu foil.
(a)
(b)
(c)
100 µm
100 µm
200 µm
Chapter 4: Results 31
As BDBA is only slightly soluble in heptanoic acid, experiments with a variety of
solvents were conducted to understand their influences on the final product. Côté, et al.1
stated that the ideal solution is one in which the BDBA precursor is moderately soluble.
As BDBA is (highly) soluble in ethanol, we attempted to dissolve the BDBA in a 1:1
solution of heptanoic acid and ethanol. The mixture proved successful and dissolved the
BDBA without sonication. The solvothermal synthesis performed however, was not
successful. Based on the IR spectrum in Figure 18, no development of the necessary
boroxine and boronate ester ring bands for COF-1 is observed. Excess peaks in the 2900
cm⁻¹ and 1800 cm⁻¹ region belong to residual heptanoic acid. Figure 19(a) and Figure
20(a) show the final morphology of a BDBA crystals produced from heptanoic acid, and
in Figure 19(b) and Figure 20(b) from the binary solvent solution.
Figure 18. IR spectrum of solvothermally annealed crystallites and precursor powder.
32 Chapter 4: Results
To examine the crystal in greater detail, and in particular to see if the crystal is a
single component or if it contains aggregates, we analysed the heptanoic/ethanol BDBA
crystal using helium ion microscopy. The analysis was unsuccessful on the heptanoic acid
only sample due to the sticky nature of the solvent, which in addition to the already highly-
insulating nature of the crystal made analysis in vacuum difficult without further heating
the sample to remove the solvent and possibly changing the crystal morphology
altogether. The heptanoic acid/ethanol solution was more cooperative, possibly due to less
(a)
(b)
100 µm
100 µm
Figure 19. COF-1 crystallites imaged using a polarizing light microscope; (a) sample prepared
using heptanoic acid solution; (b) sample prepared using heptanoic acid-ethanol solution.
(a)
(b)
40 µm
40 µm
Figure 20. COF-1 crystallites imaged using SEM; (a) sample prepared using heptanoic acid
solution; (b) sample prepared using heptanoic acid-ethanol solution.
Chapter 4: Results 33
heptanoic acid in the system or the esterification creating a solvent with a higher vapour
pressure.
As shown in Figure 21, tens of layers of crystallites build on each other to form a
single, rigidly crafted heptanoic acid/ethanol-produced BDBA aggregate. We found that,
in general, the morphology of the crystallites/aggregates formed was extremely sensitive
to the solvents used. Numerous studies have demonstrated that solvents have a significant
impact on the strength of the intermolecular forces on the faces of the solute crystal. In
other words, the solvent-crystal surface combination determines the bonds affected and
subsequently the final crystal shape and aspect ratio.156,157 Figure 22(a) illustrates the
crystal morphology of an ethanol only solution. Furthering the experiment on solvent
effects, we dissolved BDBA in 0.5:1 heptanoic acid/ethanol, 1:1 ethanol and acetone, and
acetone, and the resulting morphologies are presented in Figure 22(b) and (c) respectively.
At the low BDBA concentration of 1 mg per 1.5 mL, solvothermal synthesis using
heptanoic acid is ineffective in converting BDBA into COF-1. Increasing the
concentration was not possible as BDBA is mostly insoluble in heptanoic acid and a
moderately soluble solvent is instead required for the condensation reaction to lead to the
production of COF-1. While the heptanoic acid/ethanol solution was more soluble,
allowing the dissolving of up to 60 mg of BDBA per 1.5 mL of solvent, we observed a
similar IR spectrum as to that of the heptanoic only solution in Figure 18.
Chapter 4: Results 35
(a)
(a)
(b)
(b)
Figure 21. Heptanoic acid/ethanol solvothermal BDBA crystals high-resolution imaged using helium ion
microscopy; (a) layered crystal morphology of the heptanoic acid/ethanol treated BDBA crystal; (b) close-
up of the crystal layers.
1 µm
200 nm
(a)
(b)
(c)
(d)
Figure 22. Crystal morphologies of BDBA crystals solvothermally synthesised in various solvents imaged
using SEM; (a) ethanol, (b) 0.5:1 heptanoic acid/ethanol, (c) 1:1 ethanol/acetone, (d) acetone .
100 µm
2 µm
2 µm
1 µm
(b)
Fig
ure
18.
Hep
tano
ic
acid
/eth
anol
solv
othe
rma
l
BD
BA
crys
tals
high
-
reso
luti
on
ima
ged
usin
g
heli
um
ion
mic
rosc
opy;
(a)
laye
red
crys
tal
mor
pho
log
y of
the
hept
anoi
c
acid
/eth
anol
trea
ted
BD
BA
crys
tal;
(b)
clos
e-
up
of
the
crys
tal
laye
rs.(
b)
(a)
(a)
36 Chapter 4: Results
4.2 SONICATION
The second technique we explored was inspired by the fabrication of COF-1 and
COF-5 bulk powder via sonochemical synthesis by Yang et al. in 2012.158 Sonication
involves the transformation of the ultrasonic waves into mechanical energy by
inducing pressure variations large enough to cause bubble cavitation collapse in
liquids.159 This technique has become particularly utilised in pharmaceutical research
for its effectiveness in particle emulsification, activation and deagglomeration.153
Based on the work of Yang et al.158, we expected solovochemical treatment to act as a
one-step synthesis, directly forming COF-1 on the surface of samples.
To synthesise a substrate-confined COF-1 film via ultrasonication, the substrate
must be resistant to destruction by (1) ultrasonic waves, and (2) immersion in
heptanoic acid for more than two hours. We tested on the HOPG, SiO2/Si wafer and
graphene on Cu foil and found the foil to be most resistant to disintegration. The HOPG
was shredded almost instantly by the ultrasound, due to the intense mechanical energy
produced breaking the layers of graphite sheets, causing them to exfoliate. Crystals did
not grow at all on the Si wafer. Figure 23(a) presents the graphene on Cu foil sample
after two hours of sonication. We can see that the crystals covered the film with a
uniformity similar to solvothermal synthesis. The agglomeration of crystals at the
bottom and side of the substrate might be due to contact with the glass vial, which
could induce nucleation more vigorously than in regions only in contact with the
solvent. The crystals have a turquoise tint, which we hypothesize to be due to the
leeching of copper +2 ions from the foil due to interaction with the heptanoic acid.
Figure 23(b) shows the result of the second experiment using the same vial of solution,
which was found to have a turquoise tint at the end of the experiment. Compared to
the first experiment, the crystals were noticeably larger, thicker, more vibrant and more
abundant. Note that the resulting shape of the substrate is due to it tearing when being
removed from the vial, not during synthesis.
Chapter 4: Results 37
We were able to retrieve a small sliver of HOPG from one of the experiments
and observe the resulting product using SEM. From observations made on the small
piece alone, it appears that crystal growth was successful and proceeded in a similar
fashion to the foil. Like the foil, crystal agglomeration is observed along the edges and
curved, exposed regions (Figure 24). Broken, damaged crystals were observed (Figure
25(b)) lying randomly on many areas of the films, along with small crystals collected
into depressions, and agglomerations in Figure 25(c). The broken crystals were
assumed to be once longer like those in Figure 23(d). These outcomes were
consistently observed in subsequent experiments, leading us to the conclusion that the
technique would not produce uniform, replicable COF-1 films on the chosen substrate
and solvent mixtures.
Figure 23. Comparing two instances of sonication of graphene on Cu foil in a vial of solution,
with the second experiment using the same vial and solution as well; (a) film morphology of
first experiment; (b) close-up of sparse crystal distribution; (c) film morphology of second
experiment; (d) close-up of crystal distribution.
(a)
(b)
(c)
(d)
3 mm3
20 µm
3 mm
20 µm
3 mm
38 Chapter 4: Results
(b)
(a)
Figure 24. Film on various substrates synthesised via ultrasonication imaged using SEM; (a) graphene on
Cu foil and (b) HOPG.
30 µm
30 µm
Figure 25. Other crystal and particle morphologies observed on a post-sonicated graphene on Cu foil
imaged through SEM; (a) blocks of crystals dispersed randomly on film; (b) crystals appearing to be
broken chunks of a much longer piece; (c) small crystals dispersed randomly on more uneven regions
of the substrates.
(b)
(a)
(c)
20 µm
40 µm
20 µm
Chapter 4: Results 39
4.3 SPIN-COATING
Spin-coating is a commonly used multi-industry technique to fabricate thin films
and film uniformity is one of its main selling points.160,161 Since uniformity of films
was clearly an issue with both drop-casting and sonication, spin-coating was an
appealing deposition technique to explore. The spin-coating experiments began with
finding the optimal speed and acceleration settings for our particular film, taking into
account solvent viscosity and volatility, precursor concentration, substrate dimension,
and solution wetting behaviour on the selected substrate. Unfortunately, this is a highly
specialised, case-by-case technique and required much trial and error to find the right
recipe. Our aim was to spin-coat a uniform wet film for subsequent solvothermal
synthesis on the hot plate.
4.3.1 Spin-coating with heptanoic acid solution
The solution of 1 mg of the 1,4 benzenediboronic acid (BDBA) monomer and
1.5 mL of heptanoic acid was added to an empty 4 mL vial. It was then placed in an
ultrasonic bath for 20 minutes to completely dissolve the BDBA powders. We
identified the ideal settings to consist of a slow initial spin for 10 seconds to cast the
solution on the substrate. If the substrate was stationary, acceleration will either break
the droplet abruptly or push the solution off the substrate completely. The next segment
is the main spin, which spreads the solution evenly and evapourates the solvent. Our
solution required a fast spin in the range of 5000 rpm. Determining this speed plays
into the balance between solvent viscosity and volatility; too fast and most if not all
the solution would have been spun off, too slow and the centrifugal force has little to
no effect on spreading the solution. Finally, we slowed the spin coater to
approximately 1000 rpm, to slow down drying to allow for longer reaction times. It is
important to note that slower speeds also increase thickness of the film, as this
thickness is inversely proportional to the spin speed squared.162 However, the concern
most pressing at this stage is uniformity and as shown in Figure 26, spin coating does
not lead to a uniform distribution of crystallites on the surface. As with the other
explored techniques, only sparse crystal coverage results.
40 Chapter 4: Results
4.3.2 Spin-coating with heptanoic acid/ethanol solution
Since solvents were found to have an effect on BDBA crystal growth and
morphology using other film preparation techniques, the experiment was performed
again using the heptanoic acid/ethanol mixture, with the spin speed adjusted for the
change in solvent properties. This was also not successful in producing a uniform film.
Before proceeding with experimenting with other solvents, the concentration of
precursor molecule was re-evaluated based on the observed density of the crystallites
on the films. While the BDBA was almost insoluble in heptanoic acid, the heptanoic
acid/ethanol mixture easily dissolved 60 mg of BDBA per 1.5mL of solvent.
Compared to 1 mg in the original solution, we began with increasing the concentration
to 10 mg per 1.5 mL solvent only. This change in solution proved to be successful in
achieving a continuous film. Figure 27(a) shows a polarized image of the film
morphology on a Si wafer, and (b) a close-up of the crystal morphology. The same
result was not achieved on the HOPG as seen in Figure 27(c) and (d), similar to the
results obtained for the heptanoic only solution.
While the continuous film was achieved, solvothermal synthesis did not help
with initiating the condensation reactions as shown in the IR spectrum in Figure 28,
which shows the traces of both precursor and synthesised film overlapping almost
perfectly. This suggests that a dry film cannot be converted to COF through a standard
solvothermal synthesis.
(b)
(a)
Figure 26. BDBA solution spin-coated on two different substrates imaged using (a) HIM on the
Si wafer and (b) SEM on the HOPG.
400 nm
100 µm
Chapter 4: Results 41
Figure 28. IR Spectra of thermally annealed spin-coated COF-1 film vs BDBA precursor powder
Figure 29: IR Spectra of thermally annealed spin-coated COF-1 film vs BDBA precursor powder
Figure 27. Comparison of films spin coated and then annealed on two different substrates. (a-b) film on Si
wafer imaged using (a) optical microscopy and (b) helium ion microscopy. (c-d) film on HOPG imaged
using (c) optical microscopy and (d) scanning electron microscopy.
(b)
(a)
(d)
(c)
10 µm
500 µm
400 nm
500 µm
42 Chapter 4: Results
4.4 THERMAL IMPRINTING
We used thermal imprinting to add directional pressure (compressive strain) to
align and densify films solution drop-casted onto a substrate. While this
nanolithography-derived method usually involves the use of a template,154,155 this
experiment only intended to take advantage of the effect of compression on thin film
growth.
20 mg of BDBA in 4 mL of heptanoic acid and ethanol mix (1:1) solution was
drop-casted on a 10×10mm Si wafer. We then spin-coated the solution. A clean
substrate was then placed directly on top of it, face down as shown in Figure 5(a). The
two substrates were secured with a Teflon tape before placing it in the imprinter. A
torque wrench was then used to secure the screws at a pre-determined torque. Finally,
the complete fitting was heated for 3 hours at 120°C on a hot plate.
Four samples were fabricated using the same solution but on different days. Shown in
the SEM images in Figure 29, there were visible differences in morphology, density
and distribution between the four experiments despite using the same precursor
molecule, solution and pressure. This can imply influence from the age of the solution
but when the experiment was repeated with a new solution and on the same day, the
same results as the previous solution were obtained. We see that crystals appear to be
preferentially forming sheets approximately perpendicular to the substrate, implying
the tendency for directionality in thermally imprinted films.
Thermal imprinting has the effect of often producing two substrate-bound films
from a single spin-coated sample. To fasten the screw top to the imprinter vessel, a
torque wrench set to a specific torque was used. While this allows for consistent
loading on all parts of the imprinter, the loading between the clean, face-down
substrate and the spin-coated substrate can vary slightly with each experiment. There
were two possible scenarios here: the clean, face-down substrate can simply press
down on the spin-coated substrate and decouple smoothly after treatment, or, it can
smear the film and the film can become adhered to it. Figure 30 shows post-synthesis
optical images of (a) a spin-coated sample and (b) the corresponding clean substrate,
showing that transfer between the spin-coated substrate and the clean one produces
similar films on both.
Chapter 4: Results 43
Some film inhomogeneity may arise from the spin-coating process. While the
films appear optically uniform, the degree of this uniformity at the nanoscale is unclear
unless analysed under high-magnification. This is not feasible as the spin-coated
sample must be placed in the imprinter immediately to prevent further drying and
morphological change of the crystals.
Thermal imprinting leads to COF-1 formation. The IR spectrum (Figure 31) of
the film reveals the formation of the double boronate ester and boroxine anhydride
bonds associated with COF-1, along with some peaks representing the precursor
molecule still present. Figure 32 shows a variety of other morphologies observed from
repeated experiments. These crystals produced the same spectra as the samples before,
suggesting that they were COF-1, but the macroscale morphologies differ from those
shown in Figure 29, suggesting that more work needed to be done to achieve consistent
outcomes.
(a)
(d)
(b)
(c)
Figure 29. SEM images of morphological variations of thermally imprinted COF-1 films on Si
substrates synthesised on four different days using the same solution; (a) layering of crystals in various
distractions; (b) crystal mass appearing to be more fused together than in (a) due to greater impact
from compression; (c) dense masses of crystals; (d) densest packing of crystals seen in all samples.
1 µm
1 µm
1 µm
1 µm
44 Chapter 4: Results
Figure 31. IR spectra of thermally imprinted COF-1 film and BDBA precursor powder.
(a)
(b)
Figure 30. Thermally imprinted COF-1 film imaged using a stereomicroscope; (a) spin-coated substrate, and
(b) clean substrate.
2 mm
2 mm
B-O
B₃O₃
Chapter 4: Results 45
4.5 A NOTE ON ANALYTICAL TECHNIQUES
In these pilot studies we were not able to take advantage of several analytical
tools such as TEM and XRD, due to the difficulty in obtaining reliable data through
these techniques.
Thin film XRD requires a film that is uniform in the area covered by the beam.
This is ideally about 10 mm in diameter. Since the substrates used were only 5 mm ×
5 mm, the next best solution would be to synthesise multiple samples and scrape off
the product to be placed in a capillary tube. Scraping off the product proved almost
impossible due to the fragility of the HOPG, Si wafers and graphene on Cu foil.
Extending the synthesis technique to a 10 mm × 10 mm substrate was also challenging,
and we made this attempt only on a Si wafer. The solution did not follow the same
wetting behaviour on a larger surface; the droplet simply retreated to its ‘comfortable’
size. The edges of the substrate, which on a 5 mm × 5 mm substrate were useful to
maintain the surface tension necessary to hold the droplet, had no impact on the 10
mm × 10 mm substrate.
Figure 32. Other morphologies observed on thermally imprinted COF-1 films imaged using SEM;
(a) leaf-like crystal growth; (b) uneven distribution of pellet-shaped crystals; (c) sparse masses of
crystal aggregations.
(a)
(b)
(c)
30 µm
1 µm
3 µm
46 Chapter 4: Results
TEM requires thickness in the nanoscale and although the crystals measured
within the range, we identified through helium ion microscopy that each crystal
aggregate is actually composed of tens of layers of smaller crystallite sheets (Figure
21(b)). Under the TEM, this showed up as an opaque blob. In addition, the insulating
nature of the crystals resulted in charging effects that made the already challenging
task of finding a single crystal within the aggregate even harder.
4.6 CONCLUSIONS
The results so far provided evidence that in addition to synthesis method,
solvent, precursor concentration and substrate choice all have considerable effects on
the final morphology of the synthesis product.
The pilot experiments also revealed other variables that may be of the same
significance but that were not explicitly investigated:
• Temperature: it was unclear as to how accurate the temperature was on the
hotplate and if that inaccuracy could have an impact on the product.
• Time: the heptanoic acid sample was still ‘wet’ at the end of the two hours of
solvothermal treatment (i.e., Solvent fumes lingered/was still potent and the film
exhibited quarter-wavelength features consistent with solvent retention), while the
ethanol sample dried within two minutes.
• Water vapour: when does the water vapour stop having an effect on crystal
growth and morphology?
• Apparatus: Côté et al.1 utilised a sealed pyrex vial. A covered petri dish with
silica gel was used instead for our solvothermal experiment.
• Pressure: the sealed Pyrex vial would have accumulated measurable pressure
in comparison to the unsealed petri dish setup. As temperature rises in the sealed
vessel, increased kinetic energy of the liquid turned to vapour molecules results also
in an increase in the vapour pressure.
• Humidity: Ambient humidity was not controlled for in all experiments.
• Deposition consistency: this is more likely to affect distribution than sheet
morphology but must be considered.
Chapter 4: Results 47
In these pilot studies, the technique and solution combinations selected did not
result in the formation of a continuous film in which the precursor molecule was
predominantly converted into COF-1. The heptanoic acid/ethanol solution was
effective for spin-coating but COF-1 formation was not achieved with subsequent
annealing. The heptanoic acid/ethanol solution was also effective for thermal
imprinting, with COF-1 formation obtained. However, a continuous film did not form,
suggesting that the concentration and/or solvent mixture still needed refining. Later
experiments used different mixtures with better results.
Chapter 5: Substrate-Supported Membranes through Thermal Processing 49
Chapter 5: Substrate-Supported
Membranes through Thermal
Processing
5.1 SOLVOTHERMAL
The heptanoic acid/ethanol solvent system used in pilot studies was not able to
dissolve more than 60 mg of precursor per 1.5 mL of solvent. Following BDBA
solubility experiments (see Section 3.1.2), we created a new solvent mixture that
dissolved up to 215 mg of BDBA per 1.5 mL of solvent. Despite this capacity, we
began with the lowest viable concentration and found 55 mg to be sufficient to form a
film. This solution was used for all experiments reported from this point onward in
this chapter unless otherwise stated.
5.1.1 Si wafer and HOPG
Using the new solvent mixture of cyclohexanone, ethanol and ether, which
allows very high concentrations of BDBA to be dissolved, the solvothermal synthesis
technique produced the film synthesised on an Si wafer shown in Figure 33(a) and (b).
Figure 33(c) is a close-up of the underside of the film in (b) imaged using SEM. The
film synthesised on HOPG is shown in Figure 34. The yellow appearance of the film
is caused by the cyclohexanone and is a common oxidation effect after opening and
storage for a long period of time. During synthesis, the cracks seen in the images were
observed to develop as soon as the rigid films formed, detaching the films from the
substrate. The top side of the film synthesised on both the Si wafer and HOPG sheet
appear smooth and lacquer-like macroscopically, with the HOPG having a more
malleable behaviour (coiling) than the Si wafer. Except for the translucent HOPG film,
the opaque films on both substrates possessed a sponge-like texture as seen in Figure
33(b). These structures were even more obvious on the films synthesised on the HOPG
substrate in Figure 34, mainly due to the films being thinner and more translucent.
SEM images revealed that these structures were indentations, as seen in the
depression-like feature at the centre of Figure 33(c). The HOPG films were flexible
and therefore appear to be more susceptible to folding.
50 Chapter 5: Substrate-Supported Membranes through Thermal Processing
(a)
(b)
(c)
Figure 33. COF-1 film on a Si wafer synthesised via thermal annealing imaged using the
stereomicroscope for (a) and (b) and SEM for (c); (a) film morphology post-synthesis; (b) sponge-like
underside of film; (c) close-up of the underside of film.
1.5 mm
2 mm
3 µm
(a)
(b)
Figure 34. COF-1 film on an HOPG substrate synthesised via thermal annealing imaged using a
stereomicroscope; (a) curled-films post-synthesis; (b) close-up of films with spherical droplets
visible.
1.5 mm
1 mm
Chapter 5: Substrate-Supported Membranes through Thermal Processing 51
A repeat experiment after distillation and filtration of the cyclohexanone
produced the results shown in the optical images in Figure 35. Apart from the centre,
the film no longer possessed the yellow tint. The underside of the film also appeared
to be free of the spherical masses. IR spectra (Figure 36) show formation of the
required boron ring group bands in COF-1, corresponding to the boroxine and boronate
ester rings.
Figure 36. IR spectrum of COF-1 film obtained by thermal
annealing with BDBA powder for comparison.
(a)
(b)
Figure 35. COF-1 film thermally annealed with distilled cyclohexanone imaged using a
stereomicroscope; (a) film morphology post-synthesis; (b) sponge-like morphology of the
underside of denser, more opaque films.
2 mm
500 µm
52 Chapter 5: Substrate-Supported Membranes through Thermal Processing
5.1.2 Ceramic crucible
The new solution was also successfully tested on a rougher and more porous
substrate, a ceramic crucible. Just like films obtained from the Si wafer and HOPG,
cracks were prevalent throughout the film. Figure 37(a) shows the smoother top side
of the film and (b) the underside of the film. Figure 37(c) presents a close-up of the
underside, which appears to be composed of small individual crystals within the main
porous wafer-like pieces. Figure 38 presents the IR spectra of various parts of the
wafer. These data indicate that the more powdery forms contain more COF-1 than the
surface of the wafer-like pieces.
5.1.3 Teflon filter paper
We also experimented on a Teflon filter paper, which unlike the ceramic
crucible, does not have walls to control solution flow. Crystal growth, despite the
uneven distribution of the film as shown in Figure 39(a) and (b), is uniform with only
Figure 38. IR spectra of the surface, underside and powder form of the COF-1 film synthesised via
thermal annealing on a ceramic crucible with BDBA powder shown for comparison.
Figure 37. COF-1 film synthesised on a ceramic crucible via thermal annealing imaged using SEM; (a)
Film morphology post-synthesis; (b) close-up of crystal growth and fractures.
(a)
(b)
10 µm
2 µm
Chapter 5: Substrate-Supported Membranes through Thermal Processing 53
one sponge-like morphology identified in (c). However, the IR spectrum in Figure 40
suggests no conversion of the BDBA to COF-1 had occurred, with the film and BDBA
powder traces overlapping each almost perfectly.
The uneven distribution of the film is due to the wetting behaviour of the solution
with respect to the Teflon filter paper. Upon drop-casting, the droplet broke apart and
formed smaller droplets across the paper. Because of the porous nature of the substrate,
the solution was absorbed and disappeared faster than on other substrates. This is not
ideal as it meant faster dispersion of solution, and faster evapouration of the solvent.
The ultimate result is premature precipitation of the BDBA, eliminating the condition
required for the formation of COF-1 networks. The uniform crystal morphology
observed is thought to be the result of both the consistent seeding scaffold that is the
filter net and abundance of the precursor molecule. However, despite the porous nature
of the substrate, cracks were still prevalent, appearing to be influenced by the thicker
nets running perpendicular and connecting the thinner fibres within the filter paper.
(a)
(d)
(b)
(c)
Figure 39. Film synthesised on a Teflon filter paper via thermal annealing imaged using SEM. (a)
continuous, smooth region of the film post-synthesis; (b) porous, sponge-like crystal morphology
dominant on film; (c) cracks appearing to be influenced by the filter web texture; (d) close -up of
the cracks.
50 µm
30 µm
8 µm
10 µm
54 Chapter 5: Substrate-Supported Membranes through Thermal Processing
5.1.4 Ceramic filter paper
Solvothermal synthesis on a ceramic filter paper resulted in a predominantly
smooth continuous film with film morphology similar to that of the Teflon filter paper.
Minimal cracking was observed as shown in Figure 41(a) with a close-up of the
fractures illustrated in (b). As on the Teflon paper, the solution did not coat the entire
surface; the droplet tightened upon contact with the ceramic substrate, suggesting that
the substrate was solvophobic. The IR spectrum obtained from this film is almost
identical to that of the Teflon paper (Figure 40), with no bonds indicative of COF-1
formation present.
Figure 40. IR spectrum of the film formed on teflon filter paper with BDBA powder
data for comparison.
Chapter 5: Substrate-Supported Membranes through Thermal Processing 55
5.2 THERMAL IMPRINTING WITH CYCLOHEXANONE SOLUTION
Using the new solution, we made another attempt at thermal imprinting. At this
stage, the spin-coater was unusable, hence another method to apply the film
homogenously was devised. We utilised the vibrations produced from an ultrasonic
bath to induce ‘crystal sorting’ on the substrate. More details can be found in Appendix
A. The result is a wafer-thin, delicate film as seen in Figure 42(a). The spherical
structures were seen again but this time, also observed under the SEM (b), (c), (d).
(a)
(b)
(c)
Figure 41. SEM images of BDBA film synthesised via solvothermal annealing on a ceramic filter
paper. (a) film morphology post-synthesis; (b) close-up of the porous, sponge-like crystal
morphology dominant on the film; (c) partial coverage of film (right) on the filter paper.
5 µm
15 µm
10 µm
56 Chapter 5: Substrate-Supported Membranes through Thermal Processing
Due to the sizes of the spherical structures observed in both the solvothermally
annealed and thermally imprinted films, we hypothesized them to have an effect on
the severity of cracks. Shrinkage from loss of moisture induces channelling of cracks,
with thickness playing a significant role on the extent of these cracks; cracks do not
propagate if the thickness is less than the length of the crack.163 A repeat experiment
left behind a film with a considerable amount of cyclohexanone still remaining (Figure
43). With further testing, it was discovered that BDBA agglomerates into clusters
when added to cyclohexanone, only dispersing and dissolving when ethanol is added
in equal parts to the cyclohexanone. The agglomerates persist even after distillation of
the cyclohexanone. This synthesis did not led to formation of COF-1, as evident in the
(a)
(d)
(b)
(c)
Figure 42. COF-1 film synthesised via thermal imprinting on an SiO₂ wafer imaged using
stereomicroscope in (a) and the SEM in (b), (c), and (d). (a) film morphology post-synthesis; (b)
spherical masses that make up the 'holey' appearance in (a); (c) close-up of connected spherical
masses; (d) interwoven crystal growth in the less 'holey' regions.
1.5 mm
10 µm
10 µm
25 µm
Chapter 5: Substrate-Supported Membranes through Thermal Processing 57
IR spectra in Figure 44. We do not observe formation of boronate ester and boroxine
anhydride peaks.
Figure 43. Repeat experiment of COF-1 film synthesised via thermal imprinting on an Si wafer imaged
using stereomicroscope in (a) and (b) and the SEM in (c), and (d). (a) film morphology post-synthesis;
(b) optical close-up of the droplet-like features; (c) details of the droplets; (d) a variation of the
droplet feature seen on a different location on the same sample.
(a)
(d)
(b)
(c)
1.5 mm
15 µm
100 µm
500 µm
58 Chapter 5: Substrate-Supported Membranes through Thermal Processing
5.3 THERMAL IMPRINTING IN THE PRESENCE OF WATER
We also attempted the thermal imprinting method with water present by placing
the thermal imprinter in a humid, enclosed chamber similar to the setup for
solvothermal synthesis in Figure 3. As the imprinter is sealed vessel, we drilled a small
hole on opposite sides of the vessel to allow for better exposure to the moisture. Three
identical samples were made and the synthesis proceeded for two hours as per previous
experiments. No films were observed to have formed on any of the three samples
(Figure 45(a)). Instead, crystallites formed in isolation, with what appears to be
deterioration/degradation in the forms of holes and webs prevalent in all of them.
Figure 44. IR spectrum of thermal imprinted film using the cyclohexanone/ethanol/ether solution vs
BDBA precursor powder to show absence of peak shifts or conversion.
Figure 45. COF-1 film synthesised via thermal imprinting with the presence of water imaged using SEM. (a)
crystal distribution post-synthesis; (b) close-up of the web-like structure of crystals due to degradation.
(b)
(a)
15 µm
1.5 µm
Chapter 5: Substrate-Supported Membranes through Thermal Processing 59
5.4 SOLVOTHERMAL SYNTHESIS ON ALUMINIUM FOIL
At this point, we refined the solution further by changing the cyclohexanone with
cyclopentanone, another cyclic ketone with one less ring member than cyclohexanone.
BDBA is more soluble in this solvent, which does not lead to formation of the crystal
agglomerates during synthesis.
We tested the new solution (cyclopentanone) on a scalable substrate, aluminium
foil. The foil was cut to many sizes: 5 mm ×5 mm, 20 mm × 20 mm, 100 mm × 100
mm, 300 mm × 300 mm and 500 mm × 500 mm. The drop-casted solution droplet
dispersed upon contact, either overflowing off the foil if there was excess solution or
spreading in a non-uniform manner across the foil on larger substrates. Unlike the Si
wafer and ceramic crucible, there were no edge barriers to contain the solution (the
edges of the Si wafer effectively hold the droplet due to tension and the ceramic
crucible has walls). However, the resulting film on aluminium foil was always
continuous and formed within five minutes. With this discovery, we experimented on
a much larger foil surface: 10 cm ×10 cm and 15 cm × 15 cm. The result was the same;
the solution proved scalable on an aluminium foil. However, the films delaminate and
as can be seen in the HIM images in Figure 46(a); they curl upon removal. In the SEM
images, a consistent 1 micron thick film is observed to have grown uniformly on the
aluminium foil. The crystal morphology is not porous-like like that on the filter papers.
They films appear to comprise an assemblage of individual crystals that form layers to
make one film entity. Furthermore, we clearly see formation of COF-1 bonds in the IR
(Figure 47).
After repeated experiments, we determined a persistent challenge: controlling
coverage and thickness uniformity with scale, since the act of drop-casting the solution
is similar to simply pouring it. To overcome this problem, we utilised the method of
dip-coating: the solution is placed in a dish big enough to fit the aluminium foil and
the foil is then submerged momentarily for coating. This is unfortunately a wasteful
technique as not only is a lot of solution needed to have the foil immersed, the solution
began gelifying due to the faster solvent evaporation rate on a large surface area, in
less than a minute, rendering it unusable after only 2 to 3 applications.
60 Chapter 5: Substrate-Supported Membranes through Thermal Processing
Figure 47. IR spectrum of COF-1 synthesised via solvothermal annealing on aluminium foil with BDBA
powder for reference.
(a)
(d)
(b)
(c)
30 µm
1 µm
100 µm
1 µm
Figure 46. COF-1 film synthesised via solvothermal annealing on aluminium foil with refined solution
imaged using HIM and SEM. (a) film morphology of film delaminated from the aluminium foil (in the
background); (b) close-up of flat region seen in (a); (c) layering of crystals on the delaminated film;
(d) fracture behaviour of films still adhered to aluminium foil.
Chapter 5: Substrate-Supported Membranes through Thermal Processing 61
5.5 CONCLUSIONS
We synthesised micron-scale COF-1 films successfully by using the new solvent
combination comprising cyclohexanone, ethanol and diethyl ether, which incorporated
an increased concentration of the precursor molecules. These films, however, were
prone to cracks, perhaps due to residual stress stemming from differing thermal
expansion coefficients of the substrate and film. Repeated experiments gave similar
results and have led to the conclusion that synthesis of COF-1 film may be more easily
optimized using a different synthesis method. One such method is described in the
following chapter.
Bibliography 63
Chapter 6: Substrate-Supported
Membranes through Solvent-
Vapour Annealing
6.1 SOLVENT-VAPOUR ANNEALING AT ROOM TEMPERATURE
To avoid some of the difficulties associated with creating homogenous, defect-
free films via solvothermal synthesis, an alternative synthesis technique was
investigated. While requiring a much longer synthesis duration, solvent-vapour
annealing requires no heat input (above room temperature), making it an attractive
alternative to solvothermal synthesis. Also, the activating component is the solvent-
vapour, which allows for a gentler and less discriminating application on the film.
6.1.1 COF-5 films
A room temperature solvent-vapour technique was proposed by Medina et al. for
the synthesis of COF-5 films on a glass slide and Si wafer;93 the films produced were
high quality, and up to 10 microns thick. Solvent-vapour annealing involves the use of
a vaporizing agent, usually a solvent, to cure the film, and in this case to polymerise
the molecules of interest. For the COF-5 film synthesis, 72 hours was required to form
the micron-scale film.
As a first step, Medina’s experiment was replicated successfully and exactly as
described. Adapting the procedure prepared by Medina et al.93, a closed environment
for solvent-vapour annealing was created using a 2 L beaker, with 15 g of indicating
silica gel and a beaker of 20 mL of anisole inside. 1.5 mL of precursor solution was
drop-cast into a low form 5 cm wide (30 mL) porcelain crucible and then placed in the
2 L beaker, which was then sealed with Parafilm and left for 48 hours. A film was
achieved on a glass slide (Figure 48), although it was somewhat cracked due to
dewetting issues and contained regions of different colours. The blotchiness resulting
from the cracks appeared to not have a significant effect on the overall uniformity at
high magnification as seen in Figure 48(c); web-like porous structures were observed
on both the brown and clear regions. A more uniform film with edge-to-edge coverage
was obtained on the Si wafer (Figure 49). Optically, the Si wafer-supported film
appeared to have a different tint compared to the film on the glass slide. On closer
64 Bibliography
inspection under the SEM, this difference is explained by the different morphology, as
the Si wafer network is denser and has regularly spaced cavities or craters.
In addition to using IR to identify COF formation through the presence of the
boronate ester rings (B-O) and the expected resonance for C-O in boroxoles, as seen
in Figure 50, differentiating a successful (COF-5) film from an unsuccessful
(crystallized precursor) one is possible with the naked eye, as shown in Figure 48.
Where the COF-5 film failed to form, the resulting product is a layer of ivory and
brown crystals homogenously distributed on the substrate. After repeated experiments,
the causes of failure were determined to be an imbalance in the BDBA to HHTP ratio,
excess moisture, a chamber volume not proportional to the amount of vaporising
solvent used, and the lack of mobility of the solvent vapours; a wide-mouthed solvent
container is most ideal.
(a)
(d)
(b)
(c)
Figure 48. COF-5 film synthesised via room temperature solvent-vapour assisted annealing on a
glass slide imaged using stereomicroscope in (a) and a close-up in (b) and the SEM in (c), and a
close-up in (d).
1 µm
5 µm
2 µm
500 µm
Bibliography 65
(d)
(b)
(c)
(a)
Figure 49. COF-5 film synthesised via room temperature solvent-vapour assisted annealing on a Si
wafer imaged using stereomicroscope in (a) and a close-up in (b) and the SEM in (c), and a close-up
in (d).
1 µm
8 µm
2 mm
500 µm
Figure 50. IR spectrum of COF-5 film synthesised via solvent-vapour annealing and the COF-5
solution.
66 Bibliography
6.1.2 COF-1
After creating the new solvent mixture of cyclohexanone/ethanol/ether, we
attempted the room temperature synthesis for COF-1. The synthesis was unsuccessful
in producing a film and Figure 52 presents the resulting morphology on the Si wafer.
This film was still wet when photographed. Globular agglomerates were very prevalent
in this particular synthesis procedure. The ethanol and ether would have evaporated
within minutes, leaving the BDBA dissolved/suspended in cyclohexanone for the rest
of the duration. As mentioned before, BDBA is mildly soluble in cyclohexanone, with
the observable outcome being clumping. The IR spectrum in Figure 53 indicates no
formation of the crucial boron-based bonds characteristic of COF-1. Having the new
solution of cyclopentanone/ethanol/ether successfully synthesised COF-1 on the
(a)
(d)
(b)
(c)
Figure 51. Crystal morphology of unsuccessful synthesis of COF-5 film via room temperature
solvent-vapour annealing imaged using imaged using stereomicroscope in (a) and (b) and the SEM in
(c), and (d). (a) film morphology post-synthesis; (b) close-up of BDBA and HHTP crystal
combination; (c) close-up of crystal growth on edge of film; (d) general crystal morphology.
100 µm
200 µm
2 mm
500 µm
Bibliography 67
aluminium foil (see Section 5.4), we made another attempt on the synthesis.
Unfortunately, it was as unsuccessful as with the cyclohexanone/ethanol/ether
solution. At this point, it was unclear if the technique simply does not work for the
COF-1 due to an intrinsic barrier (e.g., a kinetic barrier) or if the substrate was the
cause of the problem. To gain clarification, we tested on a ceramic crucible with first
the cyclohexanone solution then the cyclopentanone solution. Both syntheses proved
successful, although results were more unpredictable with the cyclohexanone solution,
possibly due to the spherical clusters affecting film continuity. Not only did we achieve
100% repeatability with the cyclopentanone solution, the film also formed as a
freestanding membrane and will be further discussed in Chapter 7.
(a)
(d)
(b)
(c)
500 µm
2 mm
150 µm
500 µm
Figure 52. Film synthesised via room temperature solvent-vapour assisted annealing on an SiO₂
wafer imaged using stereomicroscope in (a), (b), and (c) and the SEM in (d). (a) film morphology
after synthesis; (b) close-up of shield like film near the edge of substrate; (c) crystal morphology
if 'shield' was absent; (d) close-up of the maze-like structure in (a).
68 Bibliography
6.2 SOLVENT-VAPOUR ANNEALING WITH THERMAL PROCESSING
The unsuccessful synthesis of COF-1 on both the glass slide and Si wafer suggest
that the formation of COF-1 networks on these substrates may require additional
energy inputs, unlike COF-5. To test this theory, we performed the solvent-vapour
annealing with additional thermal input using the same temperature as in the
solvothermal synthesis with the cyclohexanone/ethanol/ether solution. The experiment
was successful at COF-1 conversion as shown in the IR spectrum in Figure 54. The
film formed is similar in morphology to the COF-5 formed through solvent-vapour
annealing, however residual crystals were visible on the surface in Figure 55(a), with
(b) illustrating the film homogeneity captured using a polarized microscope. The
residual crystals were then analysed using the SEM; images are presented in Figure
55(c) and (d). The crystallites appear to have assembled into masses of geometric webs
across the film. This morphology is unique and has not been produced in any of our
other synthesis approaches. The crystallites were also abundant on the film, such that
XRD analysis was finally possible on one of our samples. The XRD spectrum (Figure
56) shows a peak at approximately 2 = 2.5°, suggesting an eclipsed configuration
instead of the staggered packing, which is typical of bulk COF-1. This eclipsed
stacking, however, can be found in COF-1 after high temperature treatment such as
degassing and guest molecule removal.4 The absence of other peaks may imply that
Figure 53. IR spectrum of film synthesised via solvent-vapour annealing at room temperature with
BDBA precursor powder for comparison.
Bibliography 69
our crystal is oriented, or that our crystallites were quite small. A repeat analysis of the
same sample gave similar results.
Figure 54. IR spectrum of the COF-1 film synthesised via thermal solvent-vapour annealing with a
BDBA powder precursor spectrum for comparison.
70 Bibliography
Figure 56. XRD spectrum of COF-1 film synthesised on a Si wafer via thermal solvent-vapour annealing.
Figure 55. Surface distribution of COF-1 film synthesised on Si wafer via thermal solvent-vapour assisted
annealing imaged using an (a) optical microscope, and (b) polarizing microscope; Crystal (c) distribution
and (d) morphology imaged at high-resolution using SEM.
(d)
(b)
(c)
(a)
3 µm
5 µm
500 µm
500 µm
Bibliography 71
6.3 CONCLUSIONS
Room temperature solvent-vapour annealing is an effective but gentle technique
to synthesise micron-scale COF-5 and COF-1 films. While the film is still susceptible
to cracking, the severity is significantly reduced with respect to the COF-1 films
synthesised via solvothermal processes. This film growth behaviour is seen in samples
synthesised with the cyclohexanone/ethanol/ether solution and the
cyclopentanone/ethanol/ether solution. We attribute successful film formation to the
combination of the correct substrate and solvent choices, since films did not form on
the Si wafer but were successfully created on the ceramic crucible. The cyclohexanone
solution was also observed to be unreliable with respect to repeatability, unlike the
cyclopentanone solution. For completion however, the synthesis was repeated on the
Si wafer but with thermal input, despite the film not being a continuous micron-scale
thick film like those achieved in a ceramic crucible at room temperature.
72 Bibliography
Chapter 7: Self-Supporting COF-1
Membranes
Through multiple experiments and refinement of the solution, we successfully
synthesised COF-1 films on a ceramic crucible using two methods: solvothermal
annealing and room temperature solvent-vapour annealing. Furthermore, these films
were freestanding. In this chapter, we provide a thorough description of the properties
of the films obtained through each technique.
7.1 SYNTHESIS DETAILS
We chose the solvothermal synthesis on a hot plate technique for its
straightforwardness and ease of naked-eye observation of the film formation. To
provide a more thorough investigation and characterisation of the membrane (through
technique comparison), we utilised the room temperature solvent-vapour technique as
it has been proven to work for thin film synthesis on a substrate of the COF-5.
Solvothermal Annealing: A closed environment was established on a hotplate
by using an inverted 2 L beaker to enclose both the synthesis vessel, a low-form
porcelain crucible, and a high-form crucible (3 cm wide, 10 mL) containing 3.5 mL of
indicating silica gel containing 5 mL of DDI water. 1.5 mL of precursor solution was
drop-cast into the synthesis vessel and heated for 60 minutes at 120°C.
Room-Temperature Solvent-Vapour Annealing: Adapting the procedure
prepared by Medina et al.93, a closed environment for solvent-vapour annealing was
created using a 2 L beaker, with 15 g of indicating silica gel and a beaker of 20 mL of
anisole inside. 1.5 mL of precursor solution was drop-cast into a low form 5 cm wide
(30 mL) porcelain crucible and then placed in the 2 L beaker, which was then sealed
with Parafilm and left for 48 hours.
Various concentrations of BDBA in solution, from 1 mg to 650 mg were tested
and 165 mg of BDBA in 4.5 mL of a ternary solvent system of dry cyclopentanone,
ethanol and dry diethyl ether was found to be the minimal concentration required for
a membrane to form via both thermal and room temperature solvent-vapour annealing.
A lower concentration resulted in an emulsion-like formation with irregularly
Bibliography 73
distributed clumps of crystallites coated in cyclopentanone. The right concentration
provided molecular packing sufficient for interparticle bonding is necessary for
continuous film formation. The membrane maintains integrity indefinitely until
exposure to H2O, which is known to degrade COF-1 particles through rehydration of
the boroxine rings to boronic acid.
7.2 CHARACTERISATION OF THE FREESTANDING MEMBRANES
7.2.1 Morphological
Although both synthesis procedures produced continuous films, the films were
distinguished by several differences. The thermally annealed membrane is highly
susceptible to cracking, resulting in 3 mm to 5 mm pieces with a thickness of
approximately 120 microns by the end of synthesis. A thin, dense, lacquer-like top
layer forms rapidly in the first 30-40 minutes of synthesis and delaminates shortly after
the formation of the thicker, more porous bottom layer around the 50 minute mark.
Figure 57(a) shows a cross-sectional view of the morphology of the bottom layer of
the solvothermally annealed membrane, with a close-up of the layer shown in (b). A
similar two-layer membrane with thickness of approximately 80 microns was achieved
via vapour annealing. However, the layers of the vapour annealed membrane do not
delaminate (Figure 57(c)), with both layers remaining attached to one another post-
synthesis. Mechanical force (tapping/knocking) is required to disconnect the two
layers. Cracking of the membrane is minimal, giving membranes 10 mm to15 mm in
lateral dimension on average (based on six repeated experiments). Figure 57(d) shows
the surface morphology of the bottom layer of the vapour annealed membrane, with
Figure 55(e) shows the surface of the top layers of solvothermally annealed membrane.
The stereo-optical image (Figure 57(f)) shows that two crystal morphologies
were present in the solvent-vapour annealed sample: a continuous, homogenous
network of small crystallites and larger dendritic crystal agglomerates measuring 800
μm to 1000 μm in diameter. These larger components were relatively evenly
distributed and comprise approximately 60% of the groundmass. In contrast, the
thermally annealed membrane surface is generally smooth and lacks the crystal
aggregations (Figure 57(b)). The AFM images in Figure 58 reveal similar
morphologies at the nanoscale: the solvothermally annealed sample, shown in (a), is
flat and comprises ~50 nm grains, whereas the vapour annealed sample has smaller
74 Bibliography
(~20 nm grains) which were amalgamated into aggregates that impart nanoscale
roughness.
(d)
(b)
(c)
(e)
(f)
(a)
2 mm
200 µm
100 µm
20 µm
10 µm
50 µm
Figure 57. COF-1 self-supporting membranes synthesised via thermal annealing and vapour annealing. (a)
cross-section of bottom layer of both membranes; (b) surface bottom layer of solvothermally annealed
membrane; (c) cross-section of top and bottom layer of vapour annealed membrane; (d) surface of bottom
layer of the vapour annealed membrane; (e) surface of the top bottom layer of vapour annealed; (f) stereo-
optical image of surface of top layer of solvothermally annealed membrane.
Bibliography 75
7.2.2 Crystallographic
XRD of the thermally annealed sample (Figure 59) reveals little to no BDBA
precursor, suggesting that the yield of COF-1 product was quite high. In contrast, for
the solvent-vapour sample, the BDBA peaks have a higher intensity than the COF-1
peaks. The COF-1 contributions to both spectra show peak patterns more akin to an
eclipsed stacking arrangement than the staggered COF-1 pattern observed for bulk
synthesis.1 The considerable broadening of the (100) peaks on both samples can be
attributed to disorder in the membrane stacking and to small COF-1 crystallite sizes:
Scherrer calculations suggest 107 Å crystallites for the solvothermally annealed
sample and 68 Å crystallites for the vapour annealed sample. Due to the small number
of peaks obtained in the XRD pattern, we were unable to obtain the COF to BDBA
ratio in either sample through full-pattern fitting analyses.
Figure 58. AFM phase images and roughness profile of (a) solvothermally annealed COF-1
and (b) vapour annealed COF-1 membranes
Figure 69. AFM phase images and roughness profile of (A) solvothermally annealed COF-1
76 Bibliography
7.2.3 Gas adsorption measurements
The surface areas of both membranes were determined through Ar gas
adsorption after degassing at 200 °C in N2 atmosphere for 24 hours. The measurements
were taken at 87 K from 0 to 1 Po. Isotherms (Figure 60) typical of a microporous
material were obtained for both samples, with overlapping adsorption and desorption
trends. The thermally annealed membrane has a calculated Brunauer-Emmett-Teller
(BET) surface area of 739 ± 11 m²/g, with the micropore component making up 511
m²/g and the mesopore component 228 m²/g. The solvent-vapour annealed membrane
has a surface area of 579 ± 7 m²/g, with micropore and mesopore portions of 254 m²/g
and 325 m²/g respectively. These values were obtained from the Broekhoff-De Boer t-
plot analysis. Density functional theory (DFT) modelled pore widths calculated for the
thermally annealed sample were 4 Å to 9 Å and 12 Å to 54 Å, while the solvent-vapour
annealed sample had calculated widths between 5 Å to 9 Å, 12 to 18 Å and 25 Å to 35
Å, the greater percentage in the latter two domains. In both cases we attribute the
smallest pores to the intrinsic porosity of the COF-1 solid, whereas the larger pores
likely arise from interstitial spaces between crystallites.
7.2.4 IR spectroscopy
The boronate ester B(OH)2 and boroxine anhydride (B3O3) functional bands in
both products (Figure 61) were present as expected in the 1290 cm-1 to 1340 cm-1
Solvothermal
Vapour annealed
Figure 59. XRD spectra of solvothermally annealed (blue) membrane with a sharper peak and less
evidence of unreacted BDBA than the vapour annealed (green) membrane.
Bibliography 77
range and 690 cm-1 region respectively, with the thermally annealed sample spectra
showing little to no difference pre- and post-degassing. The attenuation of
cyclopentanone peaks at the 3500 cm-1 and 1730 cm-1 regions and narrowing of the
B(OH)2 and B3O3 bands post-degassing were evident in the solvent-vapour sample. In
both samples, no significant changes were observed after degassing.
The IR spectra show an amalgamation/commingling of bands in the 1370 cm-1
to 1250 cm-1 range of B-O, C-C and C-B stretches. The B-O bands were not
symmetrical and the C-C band broadens over the C-B band, which is observed in the
Figure 60. Clean Ar gas adsorption/desorption isotherms of solvothermally annealed (blue) and
vapour annealed (green) membranes.
Figure 73. Pre-degas (darker shade) and post-degas (lighter) FT-IR spectra of TA (blue) and vapour
Figure 61. Pre-degas (darker shade) and post-degas (lighter) FT-IR spectra of TA (blue) and vapour-
annealed (green) membranes.
B-O B-C
B₃O₃
78 Bibliography
starting material. This indicates presence of the BDBA in the synthesised membrane.
The overlapping of bands can be observed in both samples but is more apparent and
extended for the vapour annealed sample before degassing.
7.2.5 Nanoindentation
Loading/unloading curves for each sample (Figure 62) were obtained from six
indents close to the center of the membrane. Instability of the probe as it loads the
surface was observed in the thermally annealed membrane, with slip pop-ins
observable from a load function as low as 500 μN. This resulted in large displacement
depths of up to 2800 nm by the end of each cycle. In contrast, a consistent loading
curve with no failure was achieved at all six indents for the solvent-vapour annealed
film, with a maximum indentation depth of 1000 nm. The evaluated modulus and
hardness of the thermally annealed sample were 2.3 GPa and 0.1 GPa, respectively,
and the values for the solvent-vapour annealed sample were 16.4 GPa and 1 GPa,
respectively.
7.3 DISCUSSION
The growth of self-supporting COF membranes comprises a number of
challenges. Solvent choice is much more critical to creating a COF membrane than it
is for producing bulk COF crystallites. For membrane formation, viscosity, substrate
wettability, and solvent volatility were all significant factors.164,165. The ternary solvent
mixtures used here produced uniform wetting of the substrates as liquids, and retained
that wetting during the polymerization/solidification process. The second major
Figure 62. Nanoindentation loading curves for (a) TA COF-1 and (b) vapour-annealed COF-1
membranes with measurement spacing matrix in onset.
Bibliography 79
challenge around COF film formation is the purity of the product. In bulk COF
synthesis, BDBA typically converts to COF-1 with a yield of about 71%,1 and
unreacted material is removed by rinsing. In micron-thick films, the unreacted
material is predominantly trapped inside the film, where it cannot be easily removed.
The value obtained for the SA sample is comparable to the value obtained by Côté et
al. 1 of 711 m²/g for bulk COF-1 powder. The SVA sample has a lower surface area,
but is within 20% of the bulk powder value. We can obtain a clearer understanding of
the difference in the surface area values from the micropore-mesopore ratios in Table
3 below:
Table 3: Micropore-Mesopore Ratio of Surface Areas
Sample Surface Area (m²/g) Micropore (%) Mesopore (%)
Côté et al. 1 711 83 17
SA-COF-1 739 70 30
SVA-COF-1 579 44 56
The bulk powder COF-1 (Côté et al.¹) has a high micropore component, with a
reported yield of 71% conversion. Although we have a slightly higher surface area for
our solvothermally annealed sample, the micropore component is 70%, which is lower
than Cote’s reported value of 87%. This could suggest a lower yield, with fewer COF-
1 micropores present and small crystallites of residual precursor leading to a high
concentration of intergrain mesopores. The low micropore proportion (46%) for the
solvent-vapour annealed sample correlates with the much lower surface area,
suggesting that the porosity dominated by intergrain mesopores, arising from the
packing of small crystallites of both COF-1 and unreacted benzenediboronic acid.
Our FTIR and XRD data support this interpretation by providing evidence of
retained BDBA. Furthermore, along with incomplete conversion from BDBA to COF-
1, guest solvent molecules were also retained within the film structure, particularly in
the vapour annealed films. Cyclopentanone is still present in the film following the
room temperature vapour annealed synthesis (Figure 61), although the degassing
procedure for gas adsorption measurements eliminates it. The XRD pattern clearly
indicates that there is more retained BDBA in the vapour annealed sample than the
80 Bibliography
solvothermally annealed sample. This implies a more efficient conversion of BDBA
to COF-1 through the thermal process and suggests that the increased temperature may
contribute to the thermal evolution of solvent from the polymer structure. However,
the solvothermally annealed membranes exhibit drawbacks in terms of their structure:
the films have two distinct morphological regimes stacked atop one another, and these
two regions of different film density tend to delaminate from one another. Further, the
film is quite prone to cracking, and has not been synthesised into large lateral
fragments comparable to the vapour annealed samples. This effect maybe correlated
with the faster evaporation and release of solvent in the solvothermally annealed
samples as compared to the vapour annealed.
The mechanical testing provides insight into the effect of these different film
morphologies, as well as elucidating the intrinsic mechanical behaviour of the
framework. The mechanical properties of single-crystal COF-1 were expected to be
highly anisotropic, and will depend critically on the orientation of the crystal. The unit
cell is unstable with respect to sheer forces along the plane of the sheets, whereas the
modulus perpendicular to the sheet direction has its maximum value of 143.7 GPa.166
Other lattice orientations exhibit values between these extremes. Microscopically, our
films comprise near randomly-oriented nanoscale crystallites, and should thus exhibit
averaged and isotropic mechanical response when measured at the film level. The
Young’s modulus and hardness of our thermally annealed sample falls in the same
range as conventional polymers whereas the solvent-vapour annealed sample is stiffer
and has a higher hardness value. Our measured results fall inside of the range of
calculated values for different crystal orientations, suggesting that the intrinsic
structure of the COF-1 contributes to their film mechanical properties. For many
materials, the mechanical response of polycrystalline materials is essentially a spatial
average of the single-crystal properties; however we cannot discount the microscopic
structure of the films as a contributor, since grain-level processes can play a role in the
mechanical response of solid materials, particularly when one of the spatial dimensions
is reduced, such as in a thin film.167-171 The macroscopic morphology of the samples
also has a significant effect on the mechanical response, as the less uniform
solvothermally annealed samples shows clear signs of slippage/breaking as compared
to the much more consistent response of the more homogeneous vapour annealed
films.
Bibliography 81
The observed difference in hardness values between the two film types might be
explained by the hardness parameter being less sensitive to substrate effects; hardness
is associated with the narrower plastic deformation region on the stress-strain curve
and the modulus with the elastic region. Despite the (twice) higher displacement depth
for the solvothermally annealed sample, substrate influence is negligible hence is not
observed in the hardness value.
The consistent measurements and higher modulus value obtained for the vapour
annealed sample can be attributed to the relatively homogeneous, continuous film
produced through this technique. Room temperature solvent-vapour annealing
involves two stages: swelling, when the solvent-vapour interacts with the deposited
material, followed by drying of the film through evaporation of the solvent,149 with
both stages being influential on the resulting crystallinity/quality of the final
product,172 and, in our procedure, each stage taking place over tens of hours. This slow
process produces a uniform, dense layer. In contrast, the thermal annealing procedure
proceeds relatively quickly, with rapid volatilization of solvents and growth of
crystallites. The presence of water vapour and the additional energy injected through
annealing allow for self-healing of the crystallites; the larger crystals and increased
yield of the solvothermally annealed process can be attributed to the presence of H2O
during thermal annealing, as H2O fosters the reversible crystallization conditions for
optimal crystallite production.1
7.4 CONCLUSIONS
We have shown that rigid, self-supporting COF-1 membranes with micron-scale
thickness can be synthesised via two different routes: solvothermal annealing and
room temperature solvent-vapour annealing. Synthesis of the membrane solely by
thermal annealing produces delicate membranes with 3 mm to 5 mm lateral sizes
whereas room temperature solvent-vapour annealing creates larger rigid membranes
10 mm to 15 mm in lateral size, although the solvent-vapour synthesis produces a
product with a significant amount of retained precursor. Both syntheses lead to films
that retain most of the porosity of bulk-synthesised COF-1. Nanoindentation results
confirm that the vapour annealed membranes were stiffer and have a higher indentation
hardness than the solvothermally annealed membranes, with a measured Young’s
modulus of 16.4 GPa. This is the first experimentally-determined value for a COF-1
film and shows that the COF properties were consistent with theoretical predictions
82 Bibliography
and significantly stiffer than conventional polymers. Maximizing the COF-1 synthesis
yield is a key step for obtaining optimal surface area, and further work is required to
determine how increasing the yield will modify the mechanical properties of the
membrane.
Bibliography 83
Chapter 8: Conclusions
This thesis presents an investigation of a range of techniques to synthesise COF-
1 and COF-5 in film form. The pilot studies in chapter 4 brought to light the various
parameters influencing film or crystallite formation. In addition to synthesis technique,
solvent, precursor concentration and choice of substrate were found to be the most
influential parameters to film formation. The solvent or solvent mixture dictates the
final crystal morphology, with precursor concentration affecting the density and
distribution of the crystals and the substrate determining the uniformity of the film
(i.e., the wetting). In addition to establishing these principles, we realized the difficulty
in preparation of these samples for analysis. Challenges included the large thickness
of the films and individual crystallites, and the film uniformity (or lack thereof), which
is crucial for methods such as XRD where a 5 mm × 5 mm uniform film is the
minimum requirement for reliable analysis. These pilot studies effectively narrowed
down the techniques for further exploration and set us on a path for the next
experiments.
Thermally processed routes to COF-1 were examined in Chapter 5. Through
this work, we see again the significance of the solvent, precursor concentration and the
substrate in film formation and the final morphology. A new solution mixture was
required to overcome the nonuniform film formation observed in the pilot studies.
Solubility studies detailed in Chapter 3 assisted in developing a solvent mixture of
cyclohexanone, ethanol and ether that not only provided the right moderately soluble
environment for the precursor but also accommodated a considerably higher
concentration of the precursor than previous solutions. This allowed us the freedom to
investigate the relationship between film formation and concentration and we
determined 55 mg per 1.5 ml of solvent to be the minimum concentration required for
a continuous film to form out of the 215 mg capacity in the ternary solvent system.
This new solution led to thick, optically visible films via solvothermal annealing and
thermal imprinting. However, the films had two issues. First, regardless of technique,
the synthesised films contained clustering of crystallites within the uniform
groundmass. The cyclohexanone was determined to be the cause of this phenomenon
and a similarly structured solvent, cyclopentanone, was found to be a good alternative.
84 Bibliography
This new solvent mixture resolved the issue and led to a cleaner, uniform film. The
second complication was film cracks, perhaps due to contrasting thermal expansion
coefficients between the substrate and film, and/or shrinkage of the film due to the
evolution of water during the synthesis. Experimenting with various substrates did not
have any effect on reducing the severity of the cracks. However, the ceramic crucible
was found to be an excellent platform for synthesizing the films as freestanding forms.
Solvent-vapour annealing methods, which require no thermal input, were
described in Chapter 6. While replication of a literature-reported synthesis was
successful for a COF-5 on a Si wafer and on glass, COF-1 films could not be formed
in the same way. However, success was achieved using a ceramic crucible as substrate,
and again, similar to the solvothermal synthesis, freestanding films were obtained and
with considerable reduction of cracks. A vapour annealing experiment with thermal
input also resulted in successful COF-1 film formation, though not of the same final
morphology (thick films). This suggests that with vapour annealing, the annealing
solvent is as important, if not more so, than substrate choice. However, further
experiments were required to confirm this hypothesis.
In Chapter 7, we describe the self-supporting membranes synthesised through
solvothermal annealing and room temperature solvent-vapour annealing. These
membranes have two layers with distinct morphologies. For the solvothermal sample,
these layers have the tendency to delaminate. Similar to the substrate-confined films,
the freestanding solvothermal membranes were appreciably more prone to cracking
than the vapour annealed membranes. XRD and FTIR data suggest a higher retention
of both solvent and precursor molecules in the vapour annealed membrane.
Mechanical testing of the membranes through nanoindentation revealed the Young's
modulus and hardness of the solvothermal sample to be 2.3 GPa and 0.1 GPa,
respectively. For the vapour annealed sample, the Young's modulus and hardness were
16.4 GPa and 1 GPa, respectively, with the latter being significantly stiffer than
conventional polymers. The successes and failures described in this work emphasize a
number of key parameters, and demonstrate the importance of solvent, substrate
choice, and precursor concentration on the formation of COF-1 films. For example,
the synthesis of COF-1 via room temperature solvent-vapour annealing did not occur
on a Si wafer but was successful on a ceramic crucible and the experiment has been
replicated over 30 times. We also observed the effect of solvent when we changed the
Bibliography 85
cyclohexanone to cyclopentanone due to the tendency for cyclohexanone to
agglomerate BDBA crystals and form globular masses sporadically incorporated into
the film. With cyclopentanone, the film produced was uniform and pristine, detaching
from the ceramic crucible cleanly without leaving behind powders like with its
predecessor, the cyclohexanone. Furthermore, the effects of BDBA precursor
concentration was observed when the formation of a macro scale freestanding COF-1
film was only achievable if BDBA concentration was above 55 mg per 1.5 mL of
solvent. Below that and only individual crystals form.
Table 3 details the experiments performed in this project in chronological order.
Each experiment was repeated at least 15 times for reliability, with those producing
conversion to COF-1 repeated and observed more rigidly.
Table 4: Syntheses in Chronological Order Synthesis
Method
Substrate Solvents and
Ratio
Precursor
per 1.5mL
solvent
Resulting
Chemistry
(through
IR)
Resulting
Morphology
1 Solvothermal Si wafer Heptanoic acid 1 mg BDBA Crystallites
2 Solvothermal HOPG Heptanoic acid 1 mg BDBA Crystallites
3 Solvothermal Si wafer Heptanoic acid /
ethanol (1:1)
1 mg BDBA Crystallites
4 Solvothermal Si wafer Heptanoic
acid/ethanol
(0.5:1)
1 mg
5 Solvothermal Si wafer Ethanol 1 mg BDBA Crystallites
6 Solvothermal Si wafer Ethanol/Acetone
(1:1)
1 mg BDBA Crystallites
7 Solvothermal Si wafer Acetone 1 mg BDBA Crystallites
8 Sonication Graphene
on Cu
Heptanoic acid 1 mg Unverified Crystallites
9 Sonication HOPG Heptanoic acid 1 mg Unverified Crystallites
10 Spin-coat then
thermal
annealing
Si wafer Heptanoic acid 1 mg BDBA Crystallites
86 Bibliography
11 Spin-coat then
thermal
annealing
HOPG Heptanoic acid 1 mg BDBA Crystallites
12 Spin-coat then
thermal
annealing
Si wafer Heptanoic acid
/ethanol
1 mg BDBA Crystallites
13 Spin-coat then
thermal
annealing
HOPG Heptanoic acid
/ethanol
1 mg BDBA Crystallites
14 Spin-coat then
thermal
annealing
Si wafer Heptanoic acid
/ethanol
10 mg BDBA Film
15 Spin-coat then
thermal
annealing
HOPG Heptanoic
acid/ethanol
10 mg BDBA Crystallites
17 Thermal
imprinting
Si wafer Heptanoic
acid/ethanol
10 mg COF-1 Partial film
19 Solvothermal Si wafer Cyclohexanone/
ethanol/ether
55 mg COF-1 Film
20 Solvothermal HOPG Cyclohexanone/
ethanol/ether
55 mg COF-1 Film
21 Thermal
Imprinting
Si wafer Cyclohexanone/
ethanol/ether
55 mg BDBA Film
22 Thermal
Imprinting w/
H2O
Si wafer Cyclohexanone/
ethanol/ether
55 mg BDBA Film
23 Solvothermal Ceramic
crucible
Cyclohexanone/
ethanol/ether
55 mg COF-1 Film
24 Solvothermal Teflon
filter paper
Cyclohexanone/
ethanol/ether
55 mg BDBA Film
25 Solvothermal Ceramic
filter paper
Cyclohexanone/
ethanol/ether
55 mg BDBA Film
26 Solvothermal Aluminiu
m foil
Cyclopentanone
/ethanol/ether
55 mg COF-1 Film
Bibliography 87
27 Room
temperature
SVA
Si wafer Acetone/ethanol
per Medina et
al.84
55 mg COF-5 Film
28 Room
temperature
SVA
Si wafer Cyclohexanone/
ethanol/ether
55 mg BDBA Film
29 Room
temperature
SVA
Si wafer Cyclopentanone
/ethanol/ether
55 mg BDBA Film
30 Room
temperature
SVA
Ceramic
crucible
Cyclohexanone/
ethanol/ether
55 mg COF-1 Film
31 Thermal SVA Si wafer Cyclohexanone/
ethanol/ether
55mg COF-1 Film
32 Solvothermal Ceramic
crucible
Cyclopentanone
/ethanol/ether
55 mg COF-1 Freestanding
film
33 Room
temperature
SVA
Ceramic
crucible
Cyclopentanone
/ethanol/ether
55 mg COF-1 Freestanding
film
Based on the work accomplished in this thesis, our future goal is to increase the COF-
1 conversion efficiency (i.e., reduce the proportion of unreacted BDBA), and increase
film size by further refining the solution and other experimental parameters such as
duration, vaporizing solvent and/or substrate. We will also extend this work on 2D-
COFs to 3D type COFs. Synthesising COFs as freestanding membranes makes them
easily integrated in engineered systems such as filtering, sensing and gas storage, and
as such these membranes may prove suitable for a range of applications.
Future Work
This Master’s project will continue to a PhD project focusing on translating/adapting
the methods developed in this project to synthesising other COF types, including
moving from 2D (plane-stacked COFs) to 3D COFs. Candidate systems will include
conducting COFs and COFs in which the reversible bonds can be converted to
irreversible bonds, which will be good candidates for a range of applications where
chemical robustness is required.
88 Bibliography
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100 Appendices
Appendices
Appendix A
Effects of Ultrasonic Vibration on Film Morphology
Figure 63 presents the setup for ultrasonic vibration assisted drop-casting of
solution on a substrate. The blank substrate is first fixed on the carbon tape. The
ultrasonic bath is then turned on and the solution drop-casted on the substrate. The
droplet will 'fizzle' systematically and as soon as the droplet disappears, the bath is
switched off and the sample moved to the next appropriate apparatus. The difference
between a sample with the solution drop-cast using this method and without post-
synthesis can be seen in Figure 64.
Figure 63. Setup of ultrasonic vibration assisted drop-casting.
Appendices 101
Figure 64. Comparison of a COF film synthesised via room temperature solvent-vapour assisted
annealing with solution drop-casted (a) and (b) with assistance from ultrasonic vibrations and (c) and
(d) without.
300 µm
300 µm
2 mm
2 mm
(a)
(d)
(c)
(b)
Fig
ure
80.
Co
mpa
riso
n of
a
CO
F
film
synt
hesi
sed
via
roo
m
tem
pera
ture
solv
ent-
vap
our
assi
sted
ann
eali
ng
with
solu
tion
dro
p-
cast
ed
(a)
and
(b)
with
assi
stan
ce
fro
m
ultr
aso
nic
vibr
atio
ns
and
(c)
and
(d)
with
out.
(b)
102 Appendices
Appendix B
COF-1: Replication of Côté et al.’s 1 method
Although our objective was to synthesise COF-1 in film form, we also made an
attempt to replicate the synthesis technique as described by Côté et al.1 for COF-1 bulk
powder. The setup is shown in Figure 65. We tested two different sized Schlenk tubes,
with both being unsuccessful as shown in the IR spectra in Figure 66, which shows
that the traces overlap perfectly with that of the precursor powder. We surmised the
failure to the following reasons:
1. Moisture may have entered at one point of the apparatus.
2. Slight overtime may have caused the reversal of COF-1 formation, but
this then must mean that this event happened very quickly. More
experiments were needed to confirm this theory.
3. Pre-existing moisture in solvents and/or precursor molecule.
(a)
(b)
(c)
Figure 65. Setup of COF-1 bulk powder synthesis via solvothermal processes.
Appendices 103
Figure 66. IR spectra of bulk powders synthesised via Côte, et al.’s1 procedure.
104 Appendices
Appendix C
For future studies: Plasma treatment of solvothermal films
The objective of this experiment was to utilise the process of carbonisation to
reduce the COF-1 band gap and eliminate the boroxine ring that makes COF-1
vulnerable in humid conditions by plasma treating the COF at room temperature and
atmospheric pressure. The sample is a COF-1 film synthesised partially via
solvothermal annealing to assure maximum film adhesion using the
cyclohexanone/ethanol/ether solvent mixture. We were able to induce morphological
changes on the film as shown but not as uniformly as we expected (Figure 67). This
could be due to the pre-existing inhomogeneity of the COF-1 film (e.g., due to
incomplete conversion and/or solvent retention) and will require further investigations.
(a)
(d)
(b)
(c)
Figure 67. Film and crystal morphology of COF-1 film synthesised via partial solvothermal annealing
and then plasma treatment. (a) film morphology after plasma-treatment; (b) colour variations of
crystals; (c) white specks appearing to outline crystal shapes; (d) dendritic-like darkening of
crystals.
3 mm
400 µm
400 µm
400 µm
Appendices 105
Appendix D
Other Morphologies Observed from Vapour Annealed COF-1 on Si Wafer
Using the Cyclohexanone/Ethanol/Ether Solution
Other Morphologies Observed from Vapour-Annealed COF-1 on Si Wafer
Using the Cyclohexanone/Ethanol/Ether Solution
(d)
(b)
(c)
(e)
(f)
(a)
Figure 68. Other crystal morphologies observed on a COF-1 film synthesised via solvent vapour annealing on a
Si wafer. (a) crystal morphology of overall film; (b) crystal morphology of the more homogenous regions; (c)
close-up of pointed edges of (b); (d) radiating agglomerates of spindle-like crystals; (e) layered, intergrowth
of shell-like structures; (f) circular-disk shaped agglomerates of crystals.
15 µm
10 µm
3 µm
30 µm
15 µm
150 µm
106 Appendices
Appendix E
Synopsis of Parameters Explored in Thesis
In detail
1. Synthesis method
a. Drop-casting
b. Solvothermal annealing
c. Sonochemical annealing
d. Solvent-vapour annealing
e. Spin-coating
f. Thermal imprinting
2. Solvents
a. Acetone
b. Cyclohexanone
c. Cyclopentanone
d. Diethyl ether
e. Ethanol
f. Heptanoic acid
3. Precursor concentration
a. 1 mg to 55 mg per 1.5 ml
4. Substrates
a. Ceramic crucible
b. Ceramic filter paper
c. Teflon filter paper
d. Glass slides
e. Graphene on Cu
f. HOPG
g. SiO₂ on Si wafer
Briefly explored (further discussed in Chapter 4 conclusion)
5. Temperature
6. Time
7. Water vapour
8. Apparatus
9. Pressure
10. Humidity
11. Deposition consistency